Author: "Alarcón, J." / Database: OAIster - Searchworks@Jio Institute Digital Library Search Results

53 results on '"Alarcón, J."'

1. Atezolizumab plus bevacizumab and chemotherapy for metastatic, persistent, or recurrent cervical cancer (BEATcc): a randomised, open-label, phase 3 trial

Author: Oaknin, A, Gladieff, L, Martínez-García, J, Villacampa, G, Takekuma, M, De Giorgi, U, Lindemann, K, Woelber, L, Colombo, N, Duska, L, Leary, A, Godoy-Ortiz, A, Nishio, S, Angelergues, A, Rubio, M, Fariñas-Madrid, L, Yamaguchi, S, Lorusso, D, Ray-Coquard, I, Manso, L, Joly, F, Alarcón, J, Follana, P, Romero, I, Lebreton, C, Pérez-Fidalgo, J, Yunokawa, M, Dahlstrand, H, D'Hondt, V, Randall, L, Oaknin, Ana, Gladieff, Laurence, Martínez-García, Jerónimo, Villacampa, Guillermo, Takekuma, Munetaka, De Giorgi, Ugo, Lindemann, Kristina, Woelber, Linn, Colombo, Nicoletta, Duska, Linda, Leary, Alexandra, Godoy-Ortiz, Ana, Nishio, Shin, Angelergues, Antoine, Rubio, Maria Jesús, Fariñas-Madrid, Lorena, Yamaguchi, Satoshi, Lorusso, Domenica, Ray-Coquard, Isabelle, Manso, Luis, Joly, Florence, Alarcón, Jesús, Follana, Philippe, Romero, Ignacio, Lebreton, Coriolan, Pérez-Fidalgo, J Alejandro, Yunokawa, Mayu, Dahlstrand, Hanna, D'Hondt, Véronique, Randall, Leslie M, Oaknin, A, Gladieff, L, Martínez-García, J, Villacampa, G, Takekuma, M, De Giorgi, U, Lindemann, K, Woelber, L, Colombo, N, Duska, L, Leary, A, Godoy-Ortiz, A, Nishio, S, Angelergues, A, Rubio, M, Fariñas-Madrid, L, Yamaguchi, S, Lorusso, D, Ray-Coquard, I, Manso, L, Joly, F, Alarcón, J, Follana, P, Romero, I, Lebreton, C, Pérez-Fidalgo, J, Yunokawa, M, Dahlstrand, H, D'Hondt, V, Randall, L, Oaknin, Ana, Gladieff, Laurence, Martínez-García, Jerónimo, Villacampa, Guillermo, Takekuma, Munetaka, De Giorgi, Ugo, Lindemann, Kristina, Woelber, Linn, Colombo, Nicoletta, Duska, Linda, Leary, Alexandra, Godoy-Ortiz, Ana, Nishio, Shin, Angelergues, Antoine, Rubio, Maria Jesús, Fariñas-Madrid, Lorena, Yamaguchi, Satoshi, Lorusso, Domenica, Ray-Coquard, Isabelle, Manso, Luis, Joly, Florence, Alarcón, Jesús, Follana, Philippe, Romero, Ignacio, Lebreton, Coriolan, Pérez-Fidalgo, J Alejandro, Yunokawa, Mayu, Dahlstrand, Hanna, D'Hondt, Véronique, and Randall, Leslie M
Abstract: Background: The GOG240 trial established bevacizumab with chemotherapy as standard first-line therapy for metastatic or recurrent cervical cancer. In the BEATcc trial (ENGOT-Cx10–GEICO 68-C–JGOG1084–GOG-3030), we aimed to evaluate the addition of an immune checkpoint inhibitor to this standard backbone. Methods: In this investigator-initiated, randomised, open-label, phase 3 trial, patients from 92 sites in Europe, Japan, and the USA with metastatic (stage IVB), persistent, or recurrent cervical cancer that was measurable, previously untreated, and not amenable to curative surgery or radiation were randomly assigned 1:1 to receive standard therapy (cisplatin 50 mg/m2 or carboplatin area under the curve of 5, paclitaxel 175 mg/m2, and bevacizumab 15 mg/kg, all on day 1 of every 3-week cycle) with or without atezolizumab 1200 mg. Treatment was continued until disease progression, unacceptable toxicity, patient withdrawal, or death. Stratification factors were previous concomitant chemoradiation (yes vs no), histology (squamous cell carcinoma vs adenocarcinoma including adenosquamous carcinoma), and platinum backbone (cisplatin vs carboplatin). Dual primary endpoints were investigator-assessed progression-free survival according to Response Evaluation Criteria in Solid Tumours version 1.1 and overall survival analysed in the intention-to-treat population. This study is registered with ClinicalTrials.gov, NCT03556839, and is ongoing. Findings: Between Oct 8, 2018, and Aug 20, 2021, 410 of 519 patients assessed for eligibility were enrolled. Median progression-free survival was 13·7 months (95% CI 12·3–16·6) with atezolizumab and 10·4 months (9·7–11·7) with standard therapy (hazard ratio [HR]=0·62 [95% CI 0·49–0·78]; p<0·0001); at the interim overall survival analysis, median overall survival was 32·1 months (95% CI 25·3–36·8) versus 22·8 months (20·3–28·0), respectively (HR 0·68 [95% CI 0·52–0·88]; p=0·0046). Grade 3 or worse adverse events occurred in 79% of patient
Published: 2024

2. Proton charge radius extraction from muon scattering at MUSE using dispersively improved chiral effective field theory

Author: Gil-Domínguez, F., Alarcón, J. M., Weiss, C., Gil-Domínguez, F., Alarcón, J. M., and Weiss, C.
Abstract: The MUSE experiment at Paul Scherrer Institute will perform the first measurement of low-energy muon-proton elastic scattering (muon lab momenta 115-210 MeV) with the aim of determining the proton charge radius. We study the prospects for the proton radius extraction using the theoretical framework of Dispersively Improved Chiral Effective Field Theory (DI$\chi$EFT). It connects the proton radii with the finite-$Q^2$ behavior of the form factors through complex analyticity and enables the use of data up to $Q^2 \sim$ 0.1 GeV$^2$ for radius extraction. We quantify the sensitivity of the $\mu p$ cross section to the proton charge radius, the theoretical uncertainty of the cross section predictions, and the size of two-photon exchange corrections. We find that the optimal kinematics for radius extraction at MUSE is at momenta 210 MeV and $Q^2 \sim$ 0.05-0.08 GeV$^2$. We compare the performance of electron and muon scattering in the same kinematics. As a byproduct, we obtain explicit predictions for the $\mu p$ and $ep$ cross sections at MUSE as functions of the assumed value of the proton radius., Comment: 12 pages, 12 figures
Published: 2023

3. Reducing the environmental impact of surgery on a global scale: systematic review and co-prioritization with healthcare workers in 132 countries

Author: Adisa, A, Bahrami-Hessari, M, Bhangu, A, George, C, Ghosh, D, Glasbey, J, Haque, P, Ingabire, J, Kamarajah, S, Kudrna, L, Ledda, V, Li, E, Lillywhite, R, Mittal, R, Nepogodiev, D, Ntirenganya, F, Picciochi, M, Simões, J, Booth, L, Elliot, R, Kennerton, A, Pettigrove, K, Pinney, L, Richard, H, Tottman, R, Wheatstone, P, Wolfenden, J, Smith, A, Sayed, A, Goswami, A, Malik, A, Mclean, A, Hassan, A, Nazimi, A, Aladna, A, Abdelgawad, A, Saed, A, Abdelmageed, A, Ghannam, A, Mahmoud, A, Alvi, A, Ismail, A, Adesunkanmi, A, Ebrahim, A, Al-Mallah, A, Alqallaf, A, Durrani, A, Gabr, A, Kirfi, A, Altaf, A, Almutairi, A, Sabbagh, A, Ajiya, A, Haddud, A, Alnsour, A, Singh, A, Mittal, A, Semple, A, Adeniran, A, Negussie, A, Oladimeji, A, Muhammad, A, Yassin, A, Gungor, A, Tarsitano, A, Soibiharry, A, Dyas, A, Frankel, A, Peckham-Cooper, A, Truss, A, Issaka, A, Ads, A, Aderogba, A, Adeyeye, A, Ademuyiwa, A, Sleem, A, Papa, A, Cordova, A, Appiah-Kubi, A, Meead, A, Nacion, A, Michael, A, Forneris, A, Duro, A, Gonzalez, A, Altouny, A, Ghazal, A, Khalifa, A, Ozair, A, Quzli, A, Haddad, A, Othman, A, Yahaya, A, Elsherbiny, A, Nazer, A, Tarek, A, Abu-Zaid, A, Al-Nusairi, A, Azab, A, Elagili, A, Elkazaz, A, Kedwany, A, Nuhu, A, Sakr, A, Shehta, A, Shirazi, A, Mohamed, A, Sherif, A, Awad, A, Abbas, A, Abdelrahman, A, Ammar, A, Azzam, A, Ciftci, A, Dural, A, Sanli, A, Rahy-Martín, A, Tantri, A, Khan, A, Al-Touny, A, Tariq, A, Gmati, A, Costas-Chavarri, A, Auerkari, A, Landaluce-Olavarria, A, Puri, A, Radhakrishnan, A, Ubom, A, Pradhan, A, Turna, A, Adepiti, A, Kuriyama, A, Kassam, A, Hassouneh, A, El-Hussuna, A, Habeebullah, A, Mousli, A, Biloslavo, A, Hoang, A, Kirk, A, Santini, A, Melero, A, Calvache, A, Baduell, A, Chan, A, Abrate, A, Balduzzi, A, Sánchez, A, Navarrete-Peón, A, Porcu, A, Brolese, A, Barranquero, A, Saibene, A, Adam, A, Vagge, A, Maquilón, A, Leon-Andrino, A, Sekulić, A, Trifunovski, A, Mako, A, Bedada, A, Broglia, A, Coppola, A, Giani, A, Grandi, A, Iacomino, A, Moro, A, D’Amico, A, Malagnino, A, Tang, A, Doyle, A, Alfieri, A, Haynes, A, Wilkins, A, Baldwin, A, Heriot, A, Laird, A, Lazarides, A, O'Connor, A, Trulson, A, Rokohl, A, Caziuc, A, Triantafyllou, A, Anesi, A, Nikova, A, Andrianakis, A, Charalabopoulos, A, Tsolakidis, A, Chirca, A, Arnaud, A, Narvaez-Rojas, A, Kavalakat, A, Spina, A, Recordare, A, Annicchiarico, A, Conti, A, Mohammed, A, Kocataş, A, Almhimid, A, Arnaout, A, Fahmy, A, Mangi, A, Modabber, A, Ulas, A, Mohamedahmed, A, Frontali, A, Moynihan, A, Yunus, A, Ahmad, A, Kent, A, Khamees, A, Ugwu, A, Turan, A, Navarro-Barrios, A, Yebes, A, De Sousa, Á, Moreno, A, Sethi, A, Dawson, A, Kaur, A, Wolde, A, Antonelli, A, Scifo, A, Alhamad, A, Davis, A, Alderazi, A, Harky, A, Mohammed-Durosinlorun, A, Seguya, A, Okhakhu, A, Chamakhi, A, Sebai, A, Souadka, A, Asla, A, Agrawal, A, Persad, A, Gupta, A, Elgazar, A, Kulkarni, A, Coates, A, Bellés, A, Hadzibegovic, A, Jotic, A, Kowark, A, Martins, A, Pineda, A, Peral, A, Gollarte, A, Senent-Boza, A, Camarena, A, Castaño-Leon, A, Bravo, A, Musina, A, Tapia-Herrero, A, Kothari, A, Raja, A, Aljaiuossi, A, Taha, A, Majbar, A, Prodromidou, A, Kanatas, A, Gupte, A, Zakaria, A, Balla, A, Barberis, A, Bondurri, A, Bottari, A, Costantino, A, Figus, A, Lauretta, A, Mingoli, A, Romanzi, A, Sagnotta, A, Scacchi, A, Picchetto, A, Valadez, A, Luzzi, A, Älgå, A, Fontalis, A, Hecker, A, Demetriades, A, Serban, A, Văcărașu, A, Cokan, A, Isaza-Restrepo, A, Beamish, A, Schache, A, Stevenson, A, Yiu, A, Cockbain, A, Litvin, A, Abad-Motos, A, Becerra, A, Ramos, Á, Chiaradia, A, Dell, A, Romano, A, Pascale, A, Marra, A, Dimas, A, Kolias, A, Cerovac, A, Koneru, A, Tidjane, A, Agbeko, A, Bajaj, A, Gosain, A, Allan, A, Carreras-Castañer, A, D'Amore, A, Dare, A, Maffioli, A, Palepa, A, Paspala, A, Konney, A, Gatta, A, Ezanno, A, Yiallourou, A, Kinnair, A, Rayner, A, Scafa, A, Bowan, A, Veglia, A, Russo, A, Maniaci, A, Castaldi, A, Gil-Moreno, A, Maffuz-Aziz, A, Meola, A, Nenna, A, Ferrer, A, Bonilla, A, Ramos-De La Medina, A, Infante, A, Santoro, A, Laganà, A, Bateman, A, Abozid, A, Seidu, A, Lowery, A, Tantraworasin, A, Rasheed, A, Picciariello, A, Isik, A, Saif, A, Anjum, A, Ioannidis, A, Abeldaño, A, Hussain, A, Nathan, A, Bedzhanyan, A, Perfecto, A, De Virgilio, A, Galvan, A, Sablotzki, A, Böttcher, A, Pellacani, A, Gatti, A, Ibrahimli, A, Menon, A, Sahni, A, Mwenda, A, Choudhry, A, Jayawardane, A, Ramasamy, A, Mitul, A, Bawa, A, Nugur, A, Rammohan, A, Sachdeva, A, Mehraj, A, Yildirim, A, Alqaseer, A, Radwan, A, Sallam, A, Syllaios, A, Tampakis, A, Alwael, A, Samara, A, Eroglu, A, Rahman, A, Ulkucu, A, Zaránd, A, Dulskas, A, Tawiah, A, Zani, A, Vas, A, Lukosiute-Urboniene, A, Adamu, A, Aujayeb, A, İplikçi, A, Mahmud, A, Cil, A, Makanjuola, A, Akwaisah, A, Galandarova, A, Saracoglu, A, Regan, A, Barlas, A, Alhassan, B, Mostafa, B, Hamida, B, Torun, B, Abdullah, B, Balagobi, B, Banky, B, Singh, B, Alegbeleye, B, Yigit, B, Hajjaj, B, Burgos-Blasco, B, Seeliger, B, Alayande, B, Alhazmi, B, Enodien, B, Torre, B, Pérez, B, Tamayo, B, De Andrés-Asenjo, B, Quintana-Villamandos, B, Girgin, B, Barmayehvar, B, Beisenov, B, Creavin, B, Dunne, B, Marson, B, Waterson, B, Martin, B, Zucker, B, Wong, B, Ozmen, B, Hammond, B, Mbwele, B, Núñez, B, Dhondt, B, Gafsi, B, Mcleish, B, Lieske, B, Tailor, B, La Pira, B, Picardi, B, Zampogna, B, Casagranda, B, Festa, B, Panda, B, Kirmani, B, Sulaiman, B, Gurung, B, Zacharia, B, Bette, B, Ayana, B, Nikolovska, B, Vilaró, B, De Vega Sánchez, B, Hameed, B, Diaconescu, B, Kovacevic, B, Bumber, B, Sakakushev, B, Tadic, B, Malek, B, Alrayes, B, Thomas, B, Gális, B, Gallagher, B, Knowles, B, Cunningham, B, Daley, B, Mishra, B, Ashford, B, Pirozzi, B, Berselli, B, Martinez-Leo, B, Sensi, B, Nardo, B, Celik, B, Giray, B, Abud, B, Almiqlash, B, Pramesh, C, Taskiran, C, De Campos Prado, C, Cipolla, C, Kumar, C, English, C, Riccetti, C, Vanni, C, Brasset, C, Downey, C, Duffy, C, Chwat, C, Cutmore, C, Sars, C, Ratto, C, Pacilio, C, De La Infiesta García, C, Moreno, C, Magalhães, C, Prada, C, Zapata, C, Senni, C, Flumignan, C, Martinez-Perez, C, Duarte, C, Garcia, C, Anderson, C, Hing, C, Cullinane, C, Cina, C, Zabkiewicz, C, Sohrabi, C, Guldogan, C, Ciubotaru, C, Desai, C, Raut, C, Demetriou, C, Handford, C, Okpani, C, Paranjape, C, Koh, C, Khatri, C, Parmar, C, Mok, C, Caricato, C, Marafante, C, Echieh, C, Tan, C, Ong, C, Conso, C, Jardinez, C, Konrads, C, Warner, C, Makwe, C, Henein, C, Fleming, C, Roland, C, Maurus, C, Nitschke, C, Mittermair, C, Mallmann, C, Andro, C, Harmston, C, Kuppler, C, Lotz, C, Nahm, C, Rowe, C, Ryalino, C, Wallis, C, Millward, C, Anthoulakis, C, Apostolou, C, Chouliaras, C, Kalfountzos, C, Kaselas, C, Vosinakis, C, Okereke, C, Chean, C, Barlow, C, Tatar, C, Clancy, C, Forde, C, Sharpin, C, Mccarthy, C, Nestor, C, Warden, C, Ávila, C, Massaguer, C, Fang, C, Martins, C, Guerci, C, Mauriello, C, Holzmeister, C, Miller, C, Weber, C, Wiesinger, C, Kenington, C, Noel, C, Sue-Chue-Lam, C, Adumah, C, Neary, C, Sen, C, Fitzgerald, C, Ezeme, C, Nastos, C, Mesina, C, Bombardini, C, Torregrosa, C, Valdespino, C, Don, C, Wickramasinghe, D, Milanesi, D, Armijos, D, Asiimwe, D, Beswick, D, Clerc, D, Cox, D, Doherty, D, Martínez, D, Lechuga, D, Gero, D, Gil-Sala, D, Lindegger, D, Reim, D, Shaerf, D, Shmukler, D, Branzan, D, Filipescu, D, Rega, D, Bernardi, D, Bissacco, D, Fusario, D, Morezzi, D, Sabella, D, Zimak, D, Vinci, D, Sale, D, Khan, D, Thereska, D, Andreotti, D, Tartaglia, D, Abdulai, D, Mukherjee, D, Verdi, D, Idowu, D, John, D, Johnson, D, Moro-Valdezate, D, Naumann, D, Omar, D, Proud, D, Roberts, D, Guzmán, D, Watson, D, Bergkvist, D, Lumenta, D, Ferrari, D, Rizzo, D, Degarege, D, Castillo, D, Douglas, D, Wright, D, Nanjiani, D, Bratus, D, Altun, D, Sievers, D, Vaysburg, D, Katechia, D, Azize, D, Rodrigues, D, Pachajoa, D, Hayne, D, Mutter, D, Raimondo, D, Eskinazi, D, Sasia, D, Corallino, D, Muduly, D, Grewal, D, Hadzhiev, D, Peristeri, D, Pournaras, D, Raptis, D, Angelou, D, Haidopoulos, D, Magouliotis, D, Moris, D, Schizas, D, Symeonidis, D, Tsironis, D, Korkolis, D, Tatsis, D, Thekkinkattil, D, Bulian, D, Pandey, D, Vatansever, D, Parker, D, Wiedemann, D, Borselle, D, Pedini, D, Schweitzer, D, Venskutonis, D, Otokwala, J, Adamu, K, Pk, P, Garod, M, Ellafi, A, Zivkovic, D, Jelovac, D, Wijeysundera, D, Mcpherson, D, Ryan, É, Ugwu, E, Baidoo, E, Shaddad, E, Memişoğlu, E, Naranjo, E, Brodkin, E, Segalini, E, Viglietta, E, Hendriks, E, Bonci, E, Sá-Marta, E, Ortega, E, Gomez, E, Joviliano, E, Clune, E, Horwell, E, Mains, E, Vasarhelyi, E, Caruana, E, Nevins, E, Yenli, E, Baili, E, Lostoridis, E, Morgan, E, Shiban, E, Latif, E, Tampaki, E, Ezenwa, E, Irune, E, Borg, E, Eisa, E, Gialamas, E, Parvez, E, Theophilidou, E, Toma, E, Arnaoutoglou, E, Samadov, E, Kantor, E, Ulman, E, Colak, E, Cassinotti, E, Bannone, E, Sarjanoja, E, Yates, E, Vincent, E, Lun, E, Cerovac, E, Dif, E, Alkhalifa, E, Daketsey, E, Fayad, E, Sheikh, E, Pontecorvi, E, Cammarata, E, La Corte, E, Rausa, E, Odai, E, Guasch, E, Cano-Trigueros, E, Uldry, E, Ros, E, Matthews, E, Donmez, E, Giorgakis, E, Kapetanakis, E, Stamatakis, E, Bua, E, Schneck, E, Nachelleh, E, Ofori, E, Akin, E, Gönüllü, E, Kirkan, E, Çelik, E, Wong, E, Capozzi, E, Pinotti, E, Colás-Ruiz, E, González, E, Fekaj, E, Ohazurike, E, Kebede, E, Erginöz, E, Duran, E, Scott, E, Aytac, E, Albanese, E, Castro, E, Albayadi, E, Kriem, E, Siddig, E, Otify, E, El Tayeb, E, Hong, E, Saguil, E, Belzile, E, Tuyishime, E, Panieri, E, Martínez, E, Myriokefalitaki, E, Samara, E, Agbeno, E, Drozdov, E, Tokidis, E, Shah, F, Barra, F, Carbone, F, Ferreli, F, Marino, F, Martinelli, F, D'Acapito, F, Masciello, F, Bàmbina, F, Issa, F, Salameh, F, Kethy, F, Mahmood, F, Gareb, F, Idrees, F, Karimian, F, Ashraf, F, Haji, F, Inayat, F, Begum, F, Nabil, F, Rosa, F, Haider, F, Parray, F, Calculli, F, Ferracci, F, Saraceno, F, Coppola, F, Coccolini, F, Fusini, F, Migliorelli, F, Pecoraro, F, Alconchel, F, Coimbra, F, Trivik-Barrientos, F, Naegele, F, Almarshad, F, Agresta, F, Fleming, F, Mendoza-Moreno, F, Brzeszczyński, F, Carannante, F, Wu, F, Aljanadi, F, Hayati, F, Campo, F, Sorbi, F, Milana, F, Takeda, F, Shekleton, F, Gessler, F, Recker, F, Grama, F, Cherbanyk, F, Faponle, F, Angelis, F, Calabretto, F, Gaino, F, Toia, F, Bianco, F, Bussu, F, Cammarata, F, Castagnini, F, Colombo, F, Ferrara, F, Fleres, F, Guerrera, F, Litta, F, Mongelli, F, Pata, F, Roscio, F, Mulita, F, Ardura, F, Tejero-Pintor, F, Calvo, F, Escobedo, F, Camacho, F, Odicino, F, Schmitt, F, Bloemers, F, Hölzle, F, Gyamfi, F, Messner, F, Koh, F, Cáceres, F, Smolle-Juettner, F, Herman, F, Ayeni, F, Djedovic, G, De Oliveira, G, Rodrigues, G, Wagner, G, Bellio, G, Giarratano, G, Capolupo, G, Budd, G, Marom, G, Poillucci, G, Thiruchandran, G, Nicholson, G, Groot, G, Hoey, G, Bass, G, Sachdev, G, Agarwal, G, Aggarwal, G, Cormio, G, Mazzarella, G, Perrone, G, 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Bussu, Francesco, Cammarata, Francesco, Castagnini, Francesco, Colombo, Francesco, Ferrara, Francesco, Fleres, Francesco, Guerrera, Francesco, Litta, Francesco, Mongelli, Francesco, Pata, Francesco, Roscio, Francesco, Mulita, Francesk, Ardura, Francisco, Tejero-Pintor, Francisco J, Calvo, Francisco Javier Redondo, Escobedo, Francisco Jose Barbosa, Camacho, Francisco José Barbosa, Odicino, Franco, Schmitt, Françoise, Bloemers, Frank, Hölzle, Frank, Gyamfi, Frank Enoch, Messner, Franka, Koh, Frederick, Cáceres, Freud, Smolle-Juettner, Freyja-Maria, Herman, Frima, Ayeni, Funbi, Djedovic, Gabriel, De Oliveira, Gabriel Paiva, Rodrigues, Gabriel, Wagner, Gabriela, Bellio, Gabriele, Giarratano, Gabriella, Capolupo, Gabriella Teresa, Budd, Gabrielle, Marom, Gad, Poillucci, Gaetano, Thiruchandran, Gajendiran, Nicholson, Gary, Groot, Gary, Hoey, Gary, Bass, Gary Alan, Sachdev, Gaurav, Agarwal, Gaurav, Aggarwal, Gaurav, Cormio, Gennaro, Mazzarella, Gennaro, Perrone, Gennaro, Osterhoff, Georg, Singer, Georg, Dejeu, George, Fowler, George, Garas, George, Gradinariu, George, Theodoropoulos, George, Tzimas, George, Babis, George, Wong, George Kwok Chu, Cross, George W V, Micha, Georgia, Chrysovitsiotis, Georgios, Koukoulis, Georgios, Peros, Georgios, Tsoulfas, Georgios, Kapetanios, Georgios, Karagiannidis, Georgios, Verras, Georgios-Ioannis, Ekwen, Gerald, Perrotta, Gerardo, Petruzzi, Gerardo, Bertelli, Giacomo, Calini, Giacomo, Fiacchini, Giacomo, Pirola, Giacomo Maria, Dolci, Giampiero, Mendiola, Gian, Baiocchi, Gian Luca, Palini, Gian Marco, Prucher, Gian Marco, D'andrea, Giancarlo, Maggiore, Giandomenico, Cassese, Gianluca, Franceschini, Gianluca, Pellino, Gianluca, Saponaro, Gianmarco, Pattacini, Gianmaria Casoni, Pantuso, Gianni, Iannella, Giannicola, Bonsaana, Gilbert Batieka, Lever, Gillian, Brachini, Gioia, Giraudo, Giorgio, Lisi, Giorgio, Russo, Giorgio Ivan, Aprea, Giovanni, Pascale, Giovanni, Tomasicchio, Giovanni, Sandri, Giovanni Battista Levi, Armatura, Giulia, Turri, Giulia, Zaccaria, Giulia, Barugola, Giuliano, Lantone, Giuliano, Gasparini, Giulio, Iacob, Giulio, Sozzi, Giulio, Zancana, Giuseppa, Mercante, Giuseppe, Bianco, Giuseppe, Brisinda, Giuseppe, Consorti, Giuseppe, Currò, Giuseppe, Giannaccare, Giuseppe, Palomba, Giuseppe, Pascarella, Giuseppe, Rotunno, Giuseppe, Spriano, Giuseppe, Vizzielli, Giuseppe, Cucinella, Giuseppe, Sica, Giuseppe, Campisi, Giuseppina, Baiocchi, Glauco, Guerra, Glen R, Pacheco, Glenda Marina Falcon, Atis, Gokhan, Augustin, Goran, Šantak, Goran, Chauhan, Govind Singh, Branagan, Graham, Harris, Grant, Stewart, Grant D, Padmore, Greg, Kocher, Gregor Jan, Di Franco, Gregorio, De Jesus Labrador Hernandez, Gregorio, Christodoulidis, Gregory, Neal-Smith, Gregory, Yim, Guang, Piozzi, Guglielmo Niccolò, Claret, Guillem, Yanowsky-Reyes, Guillermo, Dhaity, Guipson Dhaity, Cakmak, Guldeniz Karadeniz, Mohamed, Guleed, Kucuk, Gultekin Ozan, Ancans, Guntis, Banipal, Gurpreet Singh, De Bacco Marangon, Gustavo, Laporte, Gustavo, Martinez-Mier, Gustavo, Recinos, Gustavo, V, Gustavo Miguel Machain, Benshetrit, Guy, Vijgen, Guy, Pickett, Gwynedd, Rodriguez, H Alejandro, Shiwani, Haaris, Derilo, Habtamu, Awad, Hadeel, El Assaad, Hadi, Raji, Hadijat Olaide, Hardgrave, Hailey, Karakullukcu, Haluk Kerim, Abdussalam, Hameedat Opeyemi, Mustafa, Hamid, Parwaiz, Hammad, Khan, Hamza, Arbab, Hana, Naga, Hani, Salem, Hani, Ulgur, Hanife Seyda, Perez-Chrzanowska, Hanna, Greenlee, Hannah, Javanmard-Emamghissi, Hannah, Lederhuber, Hans, Osman, Hany, Adamou, Harissou, Majid, Haroon Javaid, Goor, Harry Van, Spiers, Harry V M, Manesh, Hassan Fatemi, Mushtaq, Hassan, Aljaaly, Hattan, Hasan, Hayat Ben, Ahmed, Hayat Tarig Abdelhafiz, Martinez-Said, Hector, Aguado, Héctor J, Consani, Heitor, Chaplin, Helen, Mohan, Helen, Van Vliet, Helen, Lohse, Helmut Alfredo Segovia, Shah, Hemina, Claireaux, Henry, Lule, Herman, Juara, Hernández, Abozied, Hesham, Bayo, Heura Llaquet, Alibrahim, Hidar, Kroon, Hidde M, Ulman, Hilmican, 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Madhvani, Kiran, Qin, Kirby R, Underwood, Kirk, Senanayake, Kithsiri Janakantha, Augestad, Knut Magne, Sigamoney, Kohila, Apostolou, Konstantinos, Bouchagier, Konstantinos, Bouliaris, Konstantinos, Bramis, Konstantinos, Gousias, Konstantinos, Lasithiotakis, Konstantinos, Paraskevopoulos, Konstantinos, Perivoliotis, Konstantinos, Roditis, Konstantinos, Stamatis, Konstantinos, Stroumpoulis, Konstantinos, Paraskevas, Kosmas I, Govindarajan, Krishna Kumar, Šimko, Kristián, Olson, Kristofor A, Khobragade, Krunal, Seah, Kt Matthew, Kishore, Kunal, Ayad, Kusay, Papavasiliou, Kyriakos, Angelou, Kyveli, Paniagua, Ladislao Cayetano, Czako, Ladislav, Ching, Laine Valerie Kongsun, Rai, Lajpat, Gupta, Lalit, Ismail, Lamiese, Mbodi, Langanani, Dasanayake, Lanka, Schröder, Lars, Baiyewu, Lateef Ayodele, Fortuna, Laura, Fernandez, Laura Gomez, Vivancos, Laura Guillamon, Jack, Laura, Keçi, Laura, Lavalle, Laura, Leonard, Laura, Shelmerdine, Lauren, Vaassen, Lauretta, Hasan, Layla, Lazarou, Lazaros, 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Luis Angel Suarez, Flórez, Luis Joaquín García, Capitan-Morales, Luis-Cristobal, Kowalski, Luiz Paulo, Widmer, Lukas Werner, Harper, Luke, Render, Luke, Wheldon, Luke, Abdur-Rahman, Lukman, Doğan, Lütfi, Prusty, Lydia, Katsiaras, Lykoyrgos, Gourbault, Lysander, Siddiqui, M Tayyab, Saleh, Ma'moun, Karthigeyan, Madhivanan, Rodriguez, Magdiel, Chowdhury, Mahbub, Nagappa, Mahesh, Sultania, Mahesh, Bashir, Mahmod, Alam, Mahmood, Elshahawy, Mahmoud Abdelaziz Mohamed, Elfiky, Mahmoud, Loubani, Mahmoud, Marei, Mahmoud, Mewafy, Mahmoud, Alali, Mahmoud, Nassar, Mahmoud A, Alobied, Majd, Bilfaqirah, Majed, Ahmad, Maleeha, Rius, Malena, Manangi, Mallikarjuna, Dornseifer, Mamun David, Tripathi, Manjul, S, Manjula, Sokolov, Manol, Pigeolet, Manon, Alonso, Manuel Diez, Losada, Manuel, Carretero, Manuel Moriche, Tousidonis, Manuel, Cotovio, Manuel Damasio, Wijeyaratne, Manuk, Boira, Mar Achalandabaso, Franza, Mara, Albdour, Maram, Alkhatieb, Maram, Déserts, Marc Danguy Des, Niewiera, Marc, 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Capobianco, Mattia, Di Bartolomeo, Mattia, Fehervari, Matyas, Pacilli, Maurizio, Romano, Maurizio, Zizzo, Maurizio, Domanin, Maurizio, Montuori, Mauro, Podda, Mauro, Zago, Mauro, Dzogbefia, Mawutor, Frountzas, Maximos, Thaw, May Htoo, Al-Juaifari, Maytham, Gharat, Mayur, Mohamed, Mazin, Hannan, Md Jafrul, Venketeswaran, Meenakshi, Chisthi, Meer, Dessalegn, Megbar, Kaplan, Mehmet, Çakıcı, Mehmet Çağlar, Ulutaş, Mehmet Eşref, Hassan, Mekki, Elsadek, Menan, Mengesha, Mengistu G, Gómez, Mercedes Estaire, Elbadawy, Merihan A, Pitcher, Meron, Tanal, Mert, Tokocin, Merve, Ergenç, Merve, Çelik, Meryem Nur, Bareka, Metaxia, Pekcici, Mevlut Recep, Cappuccio, Micaela, Dasa, Michael, Dewan, Michael, El Boghdady, Michael, Ezeanochie, Michael, Greenhalgh, Michael, Jenkinson, Michael, Kelly, Michael, Spartalis, Michael, Zyskowski, Michael, Racine, Michaël, De Cillia, Michael, Chu, Michael Jen Jie, Mallmann, Michael R, Zhu, Michael Z L, Klimovskij, Michail, Vailas, Michail, Kisielewski, Michał, Adamina, Michel, Campanelli, Michela, Carvello, Michele, Ammendola, Michele, Manigrasso, Michele, Scopelliti, Michele, White, Michelle, Collins, Michelle L, Chevallay, Mickael, Borges, Miguel Fróis, Mayo-Yáñez, Miguel, Melo, Miguel Rocha, Ruiz-Marín, Miguel, Eiras, Miguel Angel Freiria, Cunha, Miguel F, Pertea, Mihaela, Slavchev, Mihail, Davidescu, Mihnea, Prieto, Mikel, Agapov, Mikhail, Gahwagi, Milad, Prats, Milagros Carrasco, Rudic, Milan, Verbic, Milena Senica, Kostusiak, Milosz, Stoleriu, Mircea Gabriel, Lucas, Miriam Abellan, Barone, Mirko, Ahmad, Misbahu, Alemu, Misganaw Alemu Adimass, Fatima, Mishal, Ida, Mitsuru, Sahu, Mo, Muhaisen, Mo'nes, Salem, Moacyr, Emara, Moataz Maher, Oludara, Mobolaji, Sotudeh, Mohadeseh, Kassab, Mohamad B, Abdelkhalek, Mohamed, Alsori, Mohamed, Anwar, Mohamed, El-Kassas, Mohamed, Elbahnasawy, Mohamed, Eldabaa, Mohamed, Rabie, Mohamed, Hassanin, Mohamed Abdelghafor, Thaha, Mohamed Adhnan, Ali, Mohamed Shafi Mahboob, Alhamid, Mohammad, 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Shraddha, Abdulsalam, Shuaib, Lin, Shuxun, Hegde, Siddhi, Fiorelli, Silvia, Quaresima, Silvia, Redondo, Silvia Villacé, Palmisano, Silvia, Ruggiero, Silvia, Balogun, Simon, Cais, Simon, Cole, Simon, Federer, Simon, Le Roux, Simon, Ippoliti, Simona, Meneghini, Simona, Viola, Simona, Manfredelli, Simone, Novello, Simone, Gananadha, Sivakumar, Mesli, Smain Nabil, Kale, Smruti, Tani, Sobhana Iftekhar, Malik, Sobia, Anastasiadou, Sofia, Boligo, Sofia, Esposito, Sofia, Valanci, Sofia, Xenaki, Sofia, Pejkova, Sofija, Bandyopadhyay, Soham, Trungu, Sokol, Basu, Somprakas, Alkhatib, Sondos, Pérez-Bertólez, Sonia, Flores, Sonia Lopez, Donoghue, Sophie, Lunca, Sorinel, Orsoo, Soyombo, Potamianos, Spyridon, Devarakonda, Sreekar, Suresh, Sreelakshmi, Croghan, Stefanie M, Turi, Stefano, Capella, Stefano, Lucchini, Stefano, Magnone, Stefano, Salizzoni, Stefano, Scabini, Stefano, Scaringi, Stefano, Cioffi, Stefano Piero Bernardo, Seyfried, Steffen, Degener, Stephan, Potten, Stephanie, Taha-Mehlitz, Stephanie, Ali, Stephen, Angamuthu, Stephen, Mcaleer, Stephen, Knight, Stephen Richard, White, Stuart, Mantziari, Styliani, Kykalos, Stylianos, Goh, Su Kah, Chowdhury, Subhadip Pal, Ibrahim, Sufyan, Elzwai, Suha, Bansal, Sujesh, Tripathy, Sujit, Amrayev, Sultan, Anwar, Sumadi Lukman, Banerjee, Sumit, Thakar, Sumit, Saeed, Summaya, Venkatappa, Sunil Kumar, Das, Sunit, Techapongsatorn, Suphakarn, Dube, Surya Kumar, Lee, Susan, González-Suárez, Susana, Henriques, Susana, Konjevoda, Suzana, Gisbertz, Suzanne, Bravo, Sybil Lizanne, Mannan, Syed, Bukhari, Syed Imran, Zafar, Syed Nabeel, Batista, Sylvia, Chin, Synn Lynn, Arif, Tahera, Lawal, Taiwo Akeem, Aktokmakyan, Talar Vartanoglu, Osborn, Tamara, Szakmany, Tamas, Sztipits, Tamás, Triantafyllou, Tania, Valadez, Tania Abigail Cueto, Singh, Tanveer, Khaliq, Tanwir, Patel, Tapan, Fadalla, Tarig, Jichi, Tarik, Sammour, Tarik, Al-Shaiji, Tariq, Naggs, Taryn, Barišić, Tatjana, Nikolouzakis, Taxiarchis, Bisgin, Tayfun, Perra, Teresa, Uprak, Tevfik Kıvılcım, Dagklis, Themistoklis, Liakakos, Theodore, Sidiropoulos, Theodoros, Adjeso, Theophilus Justus Kofi, Dölker, Theresa, Oung, Thida, Aherne, Thomas, Diehl, Thomas, Pinkney, Thomas, Raymond, Thomas, Rhomberg, Thomas, Schmitz-Rixen, Thomas, Madhuri, Thumuluru Kavitha, Lohmann, Tibor Karl, Yeoh, Tien, Zaimis, Tilemachos, Bright, Tim, Vilz, Tim O, Glowka, Tim R, Board, Timothy, Hardcastle, Timothy, Cohnert, Tina, Mahečić, Tina Tomić, William, Tinka George, Klatte, Tobias, Abbott, Tom, Watcyn-Jones, Tom, Mendes, Tome, Kulis, Tomislav, Sečan, Tomislav, Campagnaro, Tommaso, Frisoni, Tommaso, Simoncini, Tommaso, Violante, Tommaso, Safranovs, Toms Janis, Risteski, Toni, Pang, Tony, Akinyemi, Tosin, Yotsov, Tsanko, Laeke, Tsegazeab, Kochiyama, Tsukasa, Sholadoye, Tunde T, Alekberli, Tural, Ezomike, Uchechukwu, Giustizieri, Ugo, Grossi, Ugo, Köksoy, Ülkü Ceren, Bork, Ulrich, Kisser, Ulrich, Ronellenfitsch, Ulrich, Saeed, Umar, Bracale, Umberto, Jayarajah, Umesh, Rauf, Umme Habiba Abdul, Bumbasirevic, Uros, Ferrer, Ursula María Jariod, Ahmed, Usama, Bello, Usman Mohammed, Jogiat, Uzair, Sadia, Uzma, Galandarov, Vagif, Narayanan, Vairavan, Calu, Valentin, Bianchi, Valentina, Ciniero, Valeria, Tonini, Valeria, Silvestri, Vania, Vijay, Vardhini, Dewan, Varun, Lohsiriwat, Varut, Thuduvage, Vasanthika, Mousafeiris, Vasileios, Dragisic, Vedran, Sasireka, Veerasamy, Santric, Veljko, Kusuma, Venkata Ramana Murthy, Kolli, Venkata Satish, Alonso, Veronica, De Simone, Veronica, Picotti, Veronica, Martínez, Verónica Martín, Panduro-Correa, Vicky, Kakotkin, Victor, Angulo, Victor Pinto, Turrado-Rodriguez, Victor, Krishnamoorthy, Vijay, Ban, Vin Shen, Shah, Vinay, Maiola, Vincenza, Giordano, Vincenzo, La Vaccara, Vincenzo, Lizzi, Vincenzo, Papagni, Vincenzo, Schiavone, Vincenzo, Satchithanantham, Vinojan, Garcia-Virto, Virginia, Jimenez, Virginia, Kumar, Vishal, Shelat, Vishal, Bhat, Vivek, Sodhai, Vivek, Graziadei, Vivien, Kutuzov, Vladislav, Stoyanov, Vladislav, Oktseloglou, Vlasios, Flis, Vojko, Elhassan, Wael Atif Fadl, Yang, Wah, Soon, Wai Cheong, Tashkandi, Wail, Al-Khyatt, Waleed, Mabood, Waleed, Bijou, Walid, Wijenayake, Wasantha, D, Wasim, Krawczyk, Wiktor, Atkins, William, Bolton, William, White, William, Ceelen, Wim, Vagena, Xanthoula, Gozal, Yaacov, Baba, Yabasin Iddrisu, Subramani, Yamini, Jansen, Yanina, Mittal, Yash, Kara, Yasi̇n, Zwain, Yasir, Noureldin, Yasser, Alawneh, Yazan, Aydin, Yener, Lam, Yick Ho, Tang, Yita, Lim, Yizhe, Dean, Yomna, Tanas, Yousef, Su, Yu-Xiong, Fujimoto, Yuki, Altinel, Yuksel, Frolova, Yulia, Oshodi, Yusuf, Fadel, Zahir T, Zahid, Zahra, Elahi, Zain, Djama, Zakarya, Zaheen, Zakia, Jawad, Zaynab, Demetrashvili, Zaza, Gebremeskel, Zersenay, Gudisa, Zewdie, Alyami, Ziyad, Garoufalia, Zoe, Li, Zoe, Zimak, Zoran, Radin, Zorana, and Balogh, Zsolt J
Abstract: Background: Healthcare cannot achieve net-zero carbon without addressing operating theatres. The aim of this study was to prioritize feasible interventions to reduce the environmental impact of operating theatres. Methods: This study adopted a four-phase Delphi consensus co-prioritization methodology. In phase 1, a systematic review of published interventions and global consultation of perioperative healthcare professionals were used to longlist interventions. In phase 2, iterative thematic analysis consolidated comparable interventions into a shortlist. In phase 3, the shortlist was coprioritized based on patient and clinician views on acceptability, feasibility, and safety. In phase 4, ranked lists of interventions were presented by their relevance to high-income countries and low-middle-income countries. Results: In phase 1, 43 interventions were identified, which had low uptake in practice according to 3042 professionals globally. In phase 2, a shortlist of 15 intervention domains was generated. In phase 3, interventions were deemed acceptable for more than 90 per cent of patients except for reducing general anaesthesia (84 per cent) and re-sterilization of 'single-use' consumables (86 per cent). In phase 4, the top three shortlisted interventions for high-income countries were: introducing recycling; reducing use of anaesthetic gases; and appropriate clinical waste processing. In phase 4, the top three shortlisted interventions for low-middle-income countries were: introducing reusable surgical devices; reducing use of consumables; and reducing the use of general anaesthesia. Conclusion: This is a step toward environmentally sustainable operating environments with actionable interventions applicable to both high- and low-middle-income countries.
Published: 2023

4. Proton charge radius extraction from muon scattering at MUSE using dispersively improved chiral effective field theory

Author: Gil-Domínguez, F., Alarcón, J. M., Weiss, C., Gil-Domínguez, F., Alarcón, J. M., and Weiss, C.
Abstract: The MUSE experiment at Paul Scherrer Institute will perform the first measurement of low-energy muon-proton elastic scattering (muon lab momenta 115-210 MeV) with the aim of determining the proton charge radius. We study the prospects for the proton radius extraction using the theoretical framework of Dispersively Improved Chiral Effective Field Theory (DI$\chi$EFT). It connects the proton radii with the finite-$Q^2$ behavior of the form factors through complex analyticity and enables the use of data up to $Q^2 \sim$ 0.1 GeV$^2$ for radius extraction. We quantify the sensitivity of the $\mu p$ cross section to the proton charge radius, the theoretical uncertainty of the cross section predictions, and the size of two-photon exchange corrections. We find that the optimal kinematics for radius extraction at MUSE is at momenta 210 MeV and $Q^2 \sim$ 0.05-0.08 GeV$^2$. We compare the performance of electron and muon scattering in the same kinematics. As a byproduct, we obtain explicit predictions for the $\mu p$ and $ep$ cross sections at MUSE as functions of the assumed value of the proton radius., Comment: 12 pages, 12 figures
Published: 2023

5. Diversity of nitrogen-removing microorganisms

Author: Franchi, O., Toledo-Alarcón, J., Campos, J.L., Jeison Nuñez, D., Vaksmaa, A., Tapia-Venegas, E., Franchi, O., Toledo-Alarcón, J., Campos, J.L., Jeison Nuñez, D., Vaksmaa, A., and Tapia-Venegas, E.
Abstract: This book chapter aims to address the microbial diversity associated with implementation prospects of nonconventional technologies for nitrogen removal in wastewater treatment plants. Special focus will be placed on the environmental advantages offered by these processes in contrast to conventional ones as heterotrophic denitrification and anammox. In addition, the operational and environmental conditions that promote the development of these microbial populations for nitrogen removal in wastewater will be addressed. Nitrate removal by an autotrophic process using sulfur compounds forms is the better characterized process and has been extensively applied in the treatment of wastewater with low C/N ratios rich in nitrates and sulfides. Hydrogenotrophic denitrification has attracted attention for application to nitrate removal from groundwater and industrial wastewater with very low organic matter content and high nitrate concentrations. This is because the process is clean, with a low biomass production and no residual organic matter. Anaerobic methanotrophic microorganisms using nitrate or nitrite (N-damo) have attracted attention for application in cooperation with anaerobic ammonia-oxidizing bacteria (anammox), resulting in the simultaneous removal of nitrogen (ammonium, nitrite, and nitrate) and methane.
Published: 2022

6. Transverse charge and current densities in the nucleon from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: Background: The transverse densities $\rho_{1, 2}(b)$ describe the distributions of electric charge and magnetic moment at fixed light-front time and connect the nucleon's elastic form factors with its partonic structure. The dispersive representation of the form factors $F_{1, 2}(t)$ expresses the densities in terms of exchanges of hadronic states in the $t$-channel and permits their analysis using hadronic physics methods. Purpose: Compute the densities at peripheral distances $b = \mathcal{O}(M_\pi^{-1})$, where they are generated predominantly by the two-pion states in the dispersive representation. Quantify the uncertainties. Methods: Dispersively improved chiral effective field theory (DI$\chi$EFT) is used to calculate the isovector spectral functions $\textrm{Im}\, F_{1, 2}(t)$ on the two-pion cut. The method includes $\pi\pi$ interactions ($\rho$ resonance) through elastic unitarity and provides realistic spectral functions up to $t \approx$ 1 GeV$^2$. Higher-mass states are parametrized by effective poles and constrained by sum rules (charges, radii, superconvergence relations). The densities $\rho_{1, 2}(b)$ are obtained from their dispersive representation. Uncertainties are quantified by varying the spectral functions. The method respects analyticity and ensures the correct $b \rightarrow \infty$ asymptotic behavior of the densities. Results: Accurate densities are obtained at all distances $b \gtrsim 0.5$ fm, with correct behavior down to $b \rightarrow 0$. The region of distances is quantified where transverse nucleon structure is governed by the two-pion state. The light-front current distributions in the polarized nucleon are computed and discussed. Conclusions: Peripheral nucleon structure can be computed from first principles using DI$\chi$EFT. The method can be extended to generalized parton distributions and other nucleon form factors., Comment: 20 pages, 12 figures, 1 table
Published: 2022

7. Brief history of the pion-nucleon sigma term

Author: Alarcón, J. M. and Alarcón, J. M.
Abstract: The pion-nucleon sigma term is a quantity involved in many important aspects of particle and nuclear physics. In this review I show its origin and how it is connected to important questions as the origin of mass of the ordinary matter, studies of dark matter detection and nucleosynthesis. I mention the most common methods used to obtain the sigma term, and comment on the extracted values. As it is shown, the accepted value of the sigma term has been moving from relatively low ($\sim 40$ MeV) to larger ones ($\sim 60$ MeV) until today, where this controversy still persist., Comment: Invited review for European Physical Journal Special Topics (REVTeX version). 34 pages, 5 figures. Accepted for publication on 10 May 2021
Published: 2022
Full Text: View/download PDF

8. Transverse charge and current densities in the nucleon from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: Background: The transverse densities $\rho_{1, 2}(b)$ describe the distributions of electric charge and magnetic moment at fixed light-front time and connect the nucleon's elastic form factors with its partonic structure. The dispersive representation of the form factors $F_{1, 2}(t)$ expresses the densities in terms of exchanges of hadronic states in the $t$-channel and permits their analysis using hadronic physics methods. Purpose: Compute the densities at peripheral distances $b = \mathcal{O}(M_\pi^{-1})$, where they are generated predominantly by the two-pion states in the dispersive representation. Quantify the uncertainties. Methods: Dispersively improved chiral effective field theory (DI$\chi$EFT) is used to calculate the isovector spectral functions $\textrm{Im}\, F_{1, 2}(t)$ on the two-pion cut. The method includes $\pi\pi$ interactions ($\rho$ resonance) through elastic unitarity and provides realistic spectral functions up to $t \approx$ 1 GeV$^2$. Higher-mass states are parametrized by effective poles and constrained by sum rules (charges, radii, superconvergence relations). The densities $\rho_{1, 2}(b)$ are obtained from their dispersive representation. Uncertainties are quantified by varying the spectral functions. The method respects analyticity and ensures the correct $b \rightarrow \infty$ asymptotic behavior of the densities. Results: Accurate densities are obtained at all distances $b \gtrsim 0.5$ fm, with correct behavior down to $b \rightarrow 0$. The region of distances is quantified where transverse nucleon structure is governed by the two-pion state. The light-front current distributions in the polarized nucleon are computed and discussed. Conclusions: Peripheral nucleon structure can be computed from first principles using DI$\chi$EFT. The method can be extended to generalized parton distributions and other nucleon form factors., Comment: 20 pages, 12 figures, 1 table
Published: 2022

9. Brief history of the pion-nucleon sigma term

Author: Alarcón, J. M. and Alarcón, J. M.
Abstract: The pion-nucleon sigma term is a quantity involved in many important aspects of particle and nuclear physics. In this review I show its origin and how it is connected to important questions as the origin of mass of the ordinary matter, studies of dark matter detection and nucleosynthesis. I mention the most common methods used to obtain the sigma term, and comment on the extracted values. As it is shown, the accepted value of the sigma term has been moving from relatively low ($\sim 40$ MeV) to larger ones ($\sim 60$ MeV) until today, where this controversy still persist., Comment: Invited review for European Physical Journal Special Topics (REVTeX version). 34 pages, 5 figures. Accepted for publication on 10 May 2021
Published: 2022
Full Text: View/download PDF

10. Nuclear matter from the ladder resummation in terms of the experimental nucleon-nucleon scattering amplitudes

Author: Alarcón, J. M., Oller, J. A., Alarcón, J. M., and Oller, J. A.
Abstract: Infinite nuclear matter is studied by resuming the series of ladder diagrams based on the results developed by us in Ann. Phys. 437, 168741 (2022). The master formula for the energy density is explicitly solved for the case of contact interactions, within a pionless description of the nucleon-nucleon interactions. Renormalized results are obtained which are directly expressed in terms of the nucleon-nucleon phase shifts and mixing angles in partial-wave amplitudes up to an including $G$ waves, with convergence reached under the inclusion of higher partial waves. The energy per particle, density and sound velocity resulting from the ladder series are given for symmetric and neutron matter. This resummation of the ladder diagrams provides a rigorous result that may be used as low-density reference for other parameterizations of $\bar{\cal{E}}$ for higher densities., Comment: 29 pages, 9 figures
Published: 2022
Full Text: View/download PDF

11. Diversity of nitrogen-removing microorganisms

Author: Franchi, O., Toledo-Alarcón, J., Campos, J.L., Jeison Nuñez, D., Vaksmaa, A., Tapia-Venegas, E., Franchi, O., Toledo-Alarcón, J., Campos, J.L., Jeison Nuñez, D., Vaksmaa, A., and Tapia-Venegas, E.
Abstract: This book chapter aims to address the microbial diversity associated with implementation prospects of nonconventional technologies for nitrogen removal in wastewater treatment plants. Special focus will be placed on the environmental advantages offered by these processes in contrast to conventional ones as heterotrophic denitrification and anammox. In addition, the operational and environmental conditions that promote the development of these microbial populations for nitrogen removal in wastewater will be addressed. Nitrate removal by an autotrophic process using sulfur compounds forms is the better characterized process and has been extensively applied in the treatment of wastewater with low C/N ratios rich in nitrates and sulfides. Hydrogenotrophic denitrification has attracted attention for application to nitrate removal from groundwater and industrial wastewater with very low organic matter content and high nitrate concentrations. This is because the process is clean, with a low biomass production and no residual organic matter. Anaerobic methanotrophic microorganisms using nitrate or nitrite (N-damo) have attracted attention for application in cooperation with anaerobic ammonia-oxidizing bacteria (anammox), resulting in the simultaneous removal of nitrogen (ammonium, nitrite, and nitrate) and methane.
Published: 2022

12. Transverse charge and current densities in the nucleon from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: Background: The transverse densities $\rho_{1, 2}(b)$ describe the distributions of electric charge and magnetic moment at fixed light-front time and connect the nucleon's elastic form factors with its partonic structure. The dispersive representation of the form factors $F_{1, 2}(t)$ expresses the densities in terms of exchanges of hadronic states in the $t$-channel and permits their analysis using hadronic physics methods. Purpose: Compute the densities at peripheral distances $b = \mathcal{O}(M_\pi^{-1})$, where they are generated predominantly by the two-pion states in the dispersive representation. Quantify the uncertainties. Methods: Dispersively improved chiral effective field theory (DI$\chi$EFT) is used to calculate the isovector spectral functions $\textrm{Im}\, F_{1, 2}(t)$ on the two-pion cut. The method includes $\pi\pi$ interactions ($\rho$ resonance) through elastic unitarity and provides realistic spectral functions up to $t \approx$ 1 GeV$^2$. Higher-mass states are parametrized by effective poles and constrained by sum rules (charges, radii, superconvergence relations). The densities $\rho_{1, 2}(b)$ are obtained from their dispersive representation. Uncertainties are quantified by varying the spectral functions. The method respects analyticity and ensures the correct $b \rightarrow \infty$ asymptotic behavior of the densities. Results: Accurate densities are obtained at all distances $b \gtrsim 0.5$ fm, with correct behavior down to $b \rightarrow 0$. The region of distances is quantified where transverse nucleon structure is governed by the two-pion state. The light-front current distributions in the polarized nucleon are computed and discussed. Conclusions: Peripheral nucleon structure can be computed from first principles using DI$\chi$EFT. The method can be extended to generalized parton distributions and other nucleon form factors., Comment: 20 pages, 12 figures, 1 table
Published: 2022
Full Text: View/download PDF

13. Brief history of the pion-nucleon sigma term

Author: Alarcón, J. M. and Alarcón, J. M.
Abstract: The pion-nucleon sigma term is a quantity involved in many important aspects of particle and nuclear physics. In this review I show its origin and how it is connected to important questions as the origin of mass of the ordinary matter, studies of dark matter detection and nucleosynthesis. I mention the most common methods used to obtain the sigma term, and comment on the extracted values. As it is shown, the accepted value of the sigma term has been moving from relatively low ($\sim 40$ MeV) to larger ones ($\sim 60$ MeV) until today, where this controversy still persist., Comment: Invited review for European Physical Journal Special Topics (REVTeX version). 34 pages, 5 figures. Accepted for publication on 10 May 2021
Published: 2022
Full Text: View/download PDF

14. Ladder resummation of spin 1/2 fermion many-body systems with arbitrary partial-wave content

Author: Alarcón, J. M., Oller, J. A., Alarcón, J. M., and Oller, J. A.
Abstract: We resum the ladder diagrams for the calculation of the energy density $\cal{E}$ of a spin 1/2 fermion many-body system in terms of arbitrary vacuum two-body scattering amplitudes. The partial-wave decomposition of the in-medium two-body scattering amplitudes is developed, and the expression for calculating $\cal{E}$ in a partial-wave amplitude expansion is also given. The case of contact interactions is completely solved and is shown to provide renormalized results, expressed directly in terms of scattering data parameters, within cutoff regularization in a wide class of schemes. $S$- and $P$-wave interactions are considered up to including the first three-terms in the effective-range expansion, paying special attention to the parametric region around the unitary limit., Comment: 58 pages, 16 figures, 2 table. New version to match the accepted manuscript in Annals of Physics. Pole content and pairing is further discussed
Published: 2021
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15. Ultracold spin-balanced fermionic quantum liquids with renormalized $P$-wave interactions

Author: Alarcón, J. M., Oller, J. A., Alarcón, J. M., and Oller, J. A.
Abstract: We consider a spin-balanced degenerate gas of spin-1/2 fermions whose dynamics is governed by low-energy $P$-wave interactions, characterized by the scattering volume $a_1$ and effective momentum $r_1$. The energy per particle $\bar{\cal{E}}$ in the many-body system is calculated by resumming the ladder diagrams comprising both particle-particle and hole-hole intermediate states, following the novel advances recently developed by us in Ann.Phys. 437,168741(2022). This allows to obtain a renormalized result for $\bar{\cal{E}}$ within generic cutoff regularization schemes, with $\bar{\cal{E}}$ directly expressed in terms of the scattering parameters $a_1$ and $r_1$, once the cut off is sent to infinity. The whole set of possible values of $a_1$ and $r_1$ is explored for the first time in the literature looking for minima in the energy per particle with $\bar{\cal{E}}$ given as described. They are actually found, but a further inspection reveals that the associated scattering parameters give rise to resonance poles in the complex momentum-plane with positive imaginary part, which is at odds with the Hermiticity of the Hamiltonian. We also determine that these conflictive poles, with a pole-position momentum that is smaller in absolute value than the Fermi momentum of the system, clearly impact the calculation of $\bar{\cal{E}}$. As a result, we conclude that unpolarized spin-1/2 fermionic normal matter interacting in $P$-wave is not stable. We also study three universal parameters around the unitary limit. Finally, the whole set of values for the parameters $a_1$, $r_1$ is characterized according to whether they give rise to unallowed poles and, if so, by attending to their pole positions relative to the Fermi momentum of the system explored., Comment: Version that matches the published one. 15 pages, 8 figures, 2 tables
Published: 2021
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16. Precise determination of proton magnetic radius from electron scattering data

Author: Alarcón, J. M., Higinbotham, D. W., Weiss, C., Alarcón, J. M., Higinbotham, D. W., and Weiss, C.
Abstract: We extract the proton magnetic radius from the high-precision electron-proton elastic scattering cross section data. Our theoretical framework combines dispersion analysis and chiral effective field theory and implements the dynamics governing the shape of the low-$Q^2$ form factors. It allows us to use data up to $Q^2\sim$ 0.5 GeV$^2$ for constraining the radii and overcomes the difficulties of empirical fits and $Q^2 \rightarrow 0$ extrapolation. We obtain a magnetic radius $r_M^p$ = 0.850 $\pm$0.001 (fit 68%) $\pm$0.010 (theory full range) fm, significantly different from earlier results obtained from the same data, and close to the extracted electric radius $r_E^p$ = 0.842 $\pm$0.002 (fit) $\pm$0.010 (theory) fm., Comment: 5 pages, 2 figures
Published: 2020
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17. Precise determination of proton magnetic radius from electron scattering data

Author: Alarcón, J. M., Higinbotham, D. W., Weiss, C., Alarcón, J. M., Higinbotham, D. W., and Weiss, C.
Abstract: We extract the proton magnetic radius from the high-precision electron-proton elastic scattering cross section data. Our theoretical framework combines dispersion analysis and chiral effective field theory and implements the dynamics governing the shape of the low-$Q^2$ form factors. It allows us to use data up to $Q^2\sim$ 0.5 GeV$^2$ for constraining the radii and overcomes the difficulties of empirical fits and $Q^2 \rightarrow 0$ extrapolation. We obtain a magnetic radius $r_M^p$ = 0.850 $\pm$0.001 (fit 68%) $\pm$0.010 (theory full range) fm, significantly different from earlier results obtained from the same data, and close to the extracted electric radius $r_E^p$ = 0.842 $\pm$0.002 (fit) $\pm$0.010 (theory) fm., Comment: 5 pages, 2 figures
Published: 2020
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18. Ripensare la scuola: esperienze e approcci di un progetto di innovazione

Author: Lorenzo Ramírez, N, Bosna, VA, Antonacci, F, Guerra, M, Vilaró Alarcón, J, Zaragozá, Pr, Bornatici, P, Carrasco Manríquez, P, López-Cassá, E, Ballesteros, G., Costa, G, Cabezas, J, Rajadell, N, Cid, R, Álvarez Bertran, N, Janer Arasa, P, Ollé, M, Mallart, J, Baqués, J, Castells, A, Soler, G, Valls, R, Lorenzo Ramìrez, N, Lorenzo Ramírez, N, Bosna, VA, Antonacci, F, Guerra, M, Vilaró Alarcón, J, Zaragozá, Pr, Bornatici, P, Carrasco Manríquez, P, López-Cassá, E, Ballesteros, G., Costa, G, Cabezas, J, Rajadell, N, Cid, R, Álvarez Bertran, N, Janer Arasa, P, Ollé, M, Mallart, J, Baqués, J, Castells, A, Soler, G, Valls, R, and Lorenzo Ramìrez, N
Abstract: A fronte dell’attuale crisi educativa, che attraversa i contesti scolastici di ogni ordine e grado a livello globale, si avverte l’urgenza di ripensare in modo radicale le teorie e i modelli che conformano più tradizionalmente la dimensione formativa. Nel capitolo vengono presentati alcuni esempi tratti da esperienze educative maturate sul territorio: si tratta di approcci e strategie che nutrono la proposta di Una scuola e che sono stati sperimentati all’interno del modello di ricerca e formazione sul campo proposto negli ultimi anni attraverso esperienze di formazione formale o informale. In particolare, da un lato, vengono approfondite metodologie che permettono di ridisegnare la scuola come contesto provocante in cui gli apprendimenti si co-costruiscono attraverso esplorazioni e domande, (Guerra 2013, 2015, 2016), dall’altro viene discusso un approccio immaginativo e ludico, che connette le diverse dimensioni dell’apprendere: cognitivo, affettivo, corporeo, mnemonico (Antonacci 2012a, 2012b; Antonacci & Rossoni, 2016).
Published: 2019

19. Proton charge radius extraction from electron scattering data using dispersively improved chiral effective field theory

Author: Alarcón, J. M., Higinbotham, D. W., Weiss, C., Ye, Z., Alarcón, J. M., Higinbotham, D. W., Weiss, C., and Ye, Z.
Abstract: We extract the proton charge radius from the elastic form factor (FF) data using a novel theoretical framework combining chiral effective field theory and dispersion analysis. Complex analyticity in the momentum transfer correlates the behavior of the spacelike FF at finite $Q^2$ with the derivative at $Q^2 = 0$. The FF calculated in the predictive theory contains the radius as a free parameter. We determine its value by comparing the predictions with a descriptive global fit of the spacelike FF data, taking into account the theoretical and experimental uncertainties. Our method allows us to use the finite-$Q^2$ FF data for constraining the radius (up to $Q^2\sim$ 0.5 GeV$^2$ and larger) and avoids the difficulties arising in methods relying on the $Q^2 \rightarrow 0$ extrapolation. We obtain a radius of 0.844(7) fm, consistent with the high-precision muonic hydrogen results., Comment: 8 pages, 5 figures
Published: 2018
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20. Accurate nucleon electromagnetic form factors from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We present a theoretical parametrization of the nucleon electromagnetic form factors (FFs) based on a combination of chiral effective field theory and dispersion analysis. The isovector spectral functions on the two-pion cut are computed using elastic unitarity, chiral pion-nucleon amplitudes, and timelike pion FF data. Higher-mass isovector and isoscalar t-channel states are described by effective poles, whose strength is fixed by sum rules (charges, radii). Excellent agreement with the spacelike proton and neutron FF data is achieved up to Q^2 \sim 1 GeV^2. Our parametrization provides proper analyticity and theoretical uncertainty estimates and can be used for low-Q^2 FF studies and proton radius extraction., Comment: 5 pages, 3 figures, 2 tables
Published: 2018
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21. Accurate nucleon electromagnetic form factors from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We present a theoretical parametrization of the nucleon electromagnetic form factors (FFs) based on a combination of chiral effective field theory and dispersion analysis. The isovector spectral functions on the two-pion cut are computed using elastic unitarity, chiral pion-nucleon amplitudes, and timelike pion FF data. Higher-mass isovector and isoscalar t-channel states are described by effective poles, whose strength is fixed by sum rules (charges, radii). Excellent agreement with the spacelike proton and neutron FF data is achieved up to Q^2 \sim 1 GeV^2. Our parametrization provides proper analyticity and theoretical uncertainty estimates and can be used for low-Q^2 FF studies and proton radius extraction., Comment: 5 pages, 3 figures, 2 tables
Published: 2018
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22. Proton charge radius extraction from electron scattering data using dispersively improved chiral effective field theory

Author: Alarcón, J. M., Higinbotham, D. W., Weiss, C., Ye, Z., Alarcón, J. M., Higinbotham, D. W., Weiss, C., and Ye, Z.
Abstract: We extract the proton charge radius from the elastic form factor (FF) data using a novel theoretical framework combining chiral effective field theory and dispersion analysis. Complex analyticity in the momentum transfer correlates the behavior of the spacelike FF at finite $Q^2$ with the derivative at $Q^2 = 0$. The FF calculated in the predictive theory contains the radius as a free parameter. We determine its value by comparing the predictions with a descriptive global fit of the spacelike FF data, taking into account the theoretical and experimental uncertainties. Our method allows us to use the finite-$Q^2$ FF data for constraining the radius (up to $Q^2\sim$ 0.5 GeV$^2$ and larger) and avoids the difficulties arising in methods relying on the $Q^2 \rightarrow 0$ extrapolation. We obtain a radius of 0.844(7) fm, consistent with the high-precision muonic hydrogen results., Comment: 8 pages, 5 figures
Published: 2018
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23. Accurate nucleon electromagnetic form factors from dispersively improved chiral effective field theory

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We present a theoretical parametrization of the nucleon electromagnetic form factors (FFs) based on a combination of chiral effective field theory and dispersion analysis. The isovector spectral functions on the two-pion cut are computed using elastic unitarity, chiral pion-nucleon amplitudes, and timelike pion FF data. Higher-mass isovector and isoscalar t-channel states are described by effective poles, whose strength is fixed by sum rules (charges, radii). Excellent agreement with the spacelike proton and neutron FF data is achieved up to Q^2 \sim 1 GeV^2. Our parametrization provides proper analyticity and theoretical uncertainty estimates and can be used for low-Q^2 FF studies and proton radius extraction., Comment: 5 pages, 3 figures, 2 tables
Published: 2018
Full Text: View/download PDF

24. Nucleon form factors in dispersively improved Chiral Effective Field Theory I: Scalar form factor

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We propose a method for calculating the nucleon form factors (FFs) of $G$-parity-even operators by combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The FFs are expressed as dispersive integrals over the two-pion cut at $t > 4 M_\pi^2$. The spectral functions are obtained from the elastic unitarity condition and expressed as products of the complex $\pi\pi \rightarrow N\bar N$ partial-wave amplitudes and the timelike pion FF. $\chi$EFT is used to calculate the ratio of the partial-wave amplitudes and the pion FF, which is real and free of $\pi\pi$ rescattering in the $t$-channel ($N/D$ method). The rescattering effects are then incorporated by multiplying with the squared modulus of the empirical pion FF. The procedure results in a marked improvement compared to conventional $\chi$EFT calculations of the spectral functions. We apply the method to the nucleon scalar FF and compute the scalar spectral function, the scalar radius, the $t$-dependent FF, and the Cheng-Dashen discrepancy. Higher-order chiral corrections are estimated through the $\pi N$ low-energy constants. Results are in excellent agreement with dispersion-theoretical calculations. We elaborate several other interesting aspects of our method. The results show proper scaling behavior in the large-$N_c$ limit of QCD because the $\chi$EFT calculation includes $N$ and $\Delta$ intermediate states. The squared modulus of the timelike pion FF required by our method can be extracted from Lattice QCD calculations of vacuum correlation functions of the operator at large Euclidean distances. Our method can be applied to the nucleon FFs of other operators of interest, such as the isovector-vector current, the energy-momentum tensor, and twist-2 QCD operators (moments of generalized parton distributions)., Comment: 17 pages and 11 figures
Published: 2017
Full Text: View/download PDF

25. Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

Author: Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, Weiss, C., Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, and Weiss, C.
Abstract: The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons. The \chi EFT calculations are extended into the \rho meson mass region using an N/D method that incorporates the pion electromagnetic form factor data. The isoscalar spectral functions are modeled by vector meson poles. We compute the peripheral charge and magnetization densities in the octet baryon states, estimate the uncertainties, and determine the quark flavor decomposition. The approach can be extended to baryon form factors of other operators and the moments of generalized parton distributions., Comment: 23 pages, 12 figures, 3 tables. Typos corrected and discussion about the anomalous thresholds added. Matches the journal version
Published: 2017
Full Text: View/download PDF

26. Nucleon form factors in dispersively improved Chiral Effective Field Theory II: Electromagnetic form factors

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We study the nucleon electromagnetic form factors (EM FFs) using a recently developed method combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The spectral functions on the two-pion cut at $t > 4 M_\pi^2$ are constructed using the elastic unitarity relation and an $N/D$ representation. $\chi$EFT is used to calculate the real functions $J_\pm^1 (t) = f_\pm^1(t)/F_\pi(t)$ (ratios of the complex $\pi\pi \rightarrow N \bar N$ partial-wave amplitudes and the timelike pion FF), which are free of $\pi\pi$ rescattering. Rescattering effects are included through the empirical timelike pion FF $|F_\pi(t)|^2$. The method allows us to compute the isovector EM spectral functions up to $t \sim 1$ GeV$^2$ with controlled accuracy (LO, NLO, and partial N2LO). With the spectral functions we calculate the isovector nucleon EM FFs and their derivatives at $t = 0$ (EM radii, moments) using subtracted dispersion relations. We predict the values of higher FF derivatives with minimal uncertainties and explain their collective behavior. We estimate the individual proton and neutron FFs by adding an empirical parametrization of the isoscalar sector. Excellent agreement with the present low-$Q^2$ FF data is achieved up to $\sim$0.5 GeV$^2$ for $G_E$, and up to $\sim$0.2 GeV$^2$ for $G_M$. Our results can be used to guide the analysis of low-$Q^2$ elastic scattering data and the extraction of the proton charge radius., Comment: 14 pages, 10 figures, 6 tables
Published: 2017
Full Text: View/download PDF

27. Nucleon form factors in dispersively improved Chiral Effective Field Theory I: Scalar form factor

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We propose a method for calculating the nucleon form factors (FFs) of $G$-parity-even operators by combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The FFs are expressed as dispersive integrals over the two-pion cut at $t > 4 M_\pi^2$. The spectral functions are obtained from the elastic unitarity condition and expressed as products of the complex $\pi\pi \rightarrow N\bar N$ partial-wave amplitudes and the timelike pion FF. $\chi$EFT is used to calculate the ratio of the partial-wave amplitudes and the pion FF, which is real and free of $\pi\pi$ rescattering in the $t$-channel ($N/D$ method). The rescattering effects are then incorporated by multiplying with the squared modulus of the empirical pion FF. The procedure results in a marked improvement compared to conventional $\chi$EFT calculations of the spectral functions. We apply the method to the nucleon scalar FF and compute the scalar spectral function, the scalar radius, the $t$-dependent FF, and the Cheng-Dashen discrepancy. Higher-order chiral corrections are estimated through the $\pi N$ low-energy constants. Results are in excellent agreement with dispersion-theoretical calculations. We elaborate several other interesting aspects of our method. The results show proper scaling behavior in the large-$N_c$ limit of QCD because the $\chi$EFT calculation includes $N$ and $\Delta$ intermediate states. The squared modulus of the timelike pion FF required by our method can be extracted from Lattice QCD calculations of vacuum correlation functions of the operator at large Euclidean distances. Our method can be applied to the nucleon FFs of other operators of interest, such as the isovector-vector current, the energy-momentum tensor, and twist-2 QCD operators (moments of generalized parton distributions)., Comment: 17 pages and 11 figures
Published: 2017
Full Text: View/download PDF

28. Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

Author: Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, Weiss, C., Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, and Weiss, C.
Abstract: The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons. The \chi EFT calculations are extended into the \rho meson mass region using an N/D method that incorporates the pion electromagnetic form factor data. The isoscalar spectral functions are modeled by vector meson poles. We compute the peripheral charge and magnetization densities in the octet baryon states, estimate the uncertainties, and determine the quark flavor decomposition. The approach can be extended to baryon form factors of other operators and the moments of generalized parton distributions., Comment: 23 pages, 12 figures, 3 tables. Typos corrected and discussion about the anomalous thresholds added. Matches the journal version
Published: 2017
Full Text: View/download PDF

29. Nucleon form factors in dispersively improved Chiral Effective Field Theory II: Electromagnetic form factors

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We study the nucleon electromagnetic form factors (EM FFs) using a recently developed method combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The spectral functions on the two-pion cut at $t > 4 M_\pi^2$ are constructed using the elastic unitarity relation and an $N/D$ representation. $\chi$EFT is used to calculate the real functions $J_\pm^1 (t) = f_\pm^1(t)/F_\pi(t)$ (ratios of the complex $\pi\pi \rightarrow N \bar N$ partial-wave amplitudes and the timelike pion FF), which are free of $\pi\pi$ rescattering. Rescattering effects are included through the empirical timelike pion FF $|F_\pi(t)|^2$. The method allows us to compute the isovector EM spectral functions up to $t \sim 1$ GeV$^2$ with controlled accuracy (LO, NLO, and partial N2LO). With the spectral functions we calculate the isovector nucleon EM FFs and their derivatives at $t = 0$ (EM radii, moments) using subtracted dispersion relations. We predict the values of higher FF derivatives with minimal uncertainties and explain their collective behavior. We estimate the individual proton and neutron FFs by adding an empirical parametrization of the isoscalar sector. Excellent agreement with the present low-$Q^2$ FF data is achieved up to $\sim$0.5 GeV$^2$ for $G_E$, and up to $\sim$0.2 GeV$^2$ for $G_M$. Our results can be used to guide the analysis of low-$Q^2$ elastic scattering data and the extraction of the proton charge radius., Comment: 14 pages, 10 figures, 6 tables
Published: 2017
Full Text: View/download PDF

30. Nucleon form factors in dispersively improved Chiral Effective Field Theory II: Electromagnetic form factors

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We study the nucleon electromagnetic form factors (EM FFs) using a recently developed method combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The spectral functions on the two-pion cut at $t > 4 M_\pi^2$ are constructed using the elastic unitarity relation and an $N/D$ representation. $\chi$EFT is used to calculate the real functions $J_\pm^1 (t) = f_\pm^1(t)/F_\pi(t)$ (ratios of the complex $\pi\pi \rightarrow N \bar N$ partial-wave amplitudes and the timelike pion FF), which are free of $\pi\pi$ rescattering. Rescattering effects are included through the empirical timelike pion FF $|F_\pi(t)|^2$. The method allows us to compute the isovector EM spectral functions up to $t \sim 1$ GeV$^2$ with controlled accuracy (LO, NLO, and partial N2LO). With the spectral functions we calculate the isovector nucleon EM FFs and their derivatives at $t = 0$ (EM radii, moments) using subtracted dispersion relations. We predict the values of higher FF derivatives with minimal uncertainties and explain their collective behavior. We estimate the individual proton and neutron FFs by adding an empirical parametrization of the isoscalar sector. Excellent agreement with the present low-$Q^2$ FF data is achieved up to $\sim$0.5 GeV$^2$ for $G_E$, and up to $\sim$0.2 GeV$^2$ for $G_M$. Our results can be used to guide the analysis of low-$Q^2$ elastic scattering data and the extraction of the proton charge radius., Comment: 14 pages, 10 figures, 6 tables
Published: 2017
Full Text: View/download PDF

31. Nucleon form factors in dispersively improved Chiral Effective Field Theory I: Scalar form factor

Author: Alarcón, J. M., Weiss, C., Alarcón, J. M., and Weiss, C.
Abstract: We propose a method for calculating the nucleon form factors (FFs) of $G$-parity-even operators by combining Chiral Effective Field Theory ($\chi$EFT) and dispersion analysis. The FFs are expressed as dispersive integrals over the two-pion cut at $t > 4 M_\pi^2$. The spectral functions are obtained from the elastic unitarity condition and expressed as products of the complex $\pi\pi \rightarrow N\bar N$ partial-wave amplitudes and the timelike pion FF. $\chi$EFT is used to calculate the ratio of the partial-wave amplitudes and the pion FF, which is real and free of $\pi\pi$ rescattering in the $t$-channel ($N/D$ method). The rescattering effects are then incorporated by multiplying with the squared modulus of the empirical pion FF. The procedure results in a marked improvement compared to conventional $\chi$EFT calculations of the spectral functions. We apply the method to the nucleon scalar FF and compute the scalar spectral function, the scalar radius, the $t$-dependent FF, and the Cheng-Dashen discrepancy. Higher-order chiral corrections are estimated through the $\pi N$ low-energy constants. Results are in excellent agreement with dispersion-theoretical calculations. We elaborate several other interesting aspects of our method. The results show proper scaling behavior in the large-$N_c$ limit of QCD because the $\chi$EFT calculation includes $N$ and $\Delta$ intermediate states. The squared modulus of the timelike pion FF required by our method can be extracted from Lattice QCD calculations of vacuum correlation functions of the operator at large Euclidean distances. Our method can be applied to the nucleon FFs of other operators of interest, such as the isovector-vector current, the energy-momentum tensor, and twist-2 QCD operators (moments of generalized parton distributions)., Comment: 17 pages and 11 figures
Published: 2017
Full Text: View/download PDF

32. Peripheral transverse densities of the baryon octet from chiral effective field theory and dispersion analysis

Author: Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, Weiss, C., Alarcón, J. M., Blin, A. N. Hiller, Vacas, M. J. Vicente, and Weiss, C.
Abstract: The baryon electromagnetic form factors are expressed in terms of two-dimensional densities describing the distribution of charge and magnetization in transverse space at fixed light-front time. We calculate the transverse densities of the spin-1/2 flavor-octet baryons at peripheral distances b = O(M_\pi^{-1}) using methods of relativistic chiral effective field theory (\chi EFT) and dispersion analysis. The densities are represented as dispersive integrals over the imaginary parts of the form factors in the timelike region (spectral functions). The isovector spectral functions on the two-pion cut t > 4 M_\pi^2 are calculated using relativistic \chi EFT including octet and decuplet baryons. The \chi EFT calculations are extended into the \rho meson mass region using an N/D method that incorporates the pion electromagnetic form factor data. The isoscalar spectral functions are modeled by vector meson poles. We compute the peripheral charge and magnetization densities in the octet baryon states, estimate the uncertainties, and determine the quark flavor decomposition. The approach can be extended to baryon form factors of other operators and the moments of generalized parton distributions., Comment: 23 pages, 12 figures, 3 tables. Typos corrected and discussion about the anomalous thresholds added. Matches the journal version
Published: 2017
Full Text: View/download PDF

33. Effects of regulated deficit irrigation on physiology, yield and fruit quality in apricot trees under Mediterranean conditions

Author: Mounzer, Oussama Hussein, Nicolás Nicolás, Emilio, Pérez Sarmiento, Francisco, Mirás-Avalos, José Manuel, Alcobendas, Rosalía, Alarcón, J., Mounzer, Oussama Hussein, Nicolás Nicolás, Emilio, Pérez Sarmiento, Francisco, Mirás-Avalos, José Manuel, Alcobendas, Rosalía, and Alarcón, J.
Abstract: Scarce water resources mainly in arid and semi-arid areas have caused an increasing interest for applying irrigation protocols aiming to reduce water spends. The effects of regulated deficit irrigation (RDI) on the performance of apricot trees (Prunus armeniaca L. cv. “Búlida”) were assessed in Murcia (SE Spain), during three consecutive growing seasons (2008-2010). The hypothesis was that RDI would not restrict yield but increase fruit quality while saving water. Two irrigation treatments were established: i) control, irrigated to fully satisfy crop water requirements (100% ETc) and ii) RDI, that reduced the amount of applied water to: a) 40% of ETc at flowering and stage I of fruit growth; b) 60% of ETc during the stage II of fruit growth and c) 50% and 25% of ETc during the late postharvest period (from 60 days after harvest). Stem water potential, gas exchanges, trunk cross-sectional area (TCSA), fruit diameter, yield and fruit quality traits were determined. Vegetative growth was decreased by the use of RDI (12% less TCSA on average for the three years), whereas yield was unaffected. In addition, some qualitative characteristics of the fruits, such as the level of soluble solids, sweetness/acidity relation and fruit colour, were improved by the use of RDI. These results and average water savings of approximately 30%, lead us to conclude that RDI strategies are a possible solution for irrigation management in areas with water shortages, such as arid and semi-arid environments.
Published: 2016

34. Algoritmo de gestión para la recarga de vehículos eléctricos

Author: Mendoza, C, Quintero, A, Alarcón, J, Mendoza, C, Quintero, A, and Alarcón, J
Abstract: This article presents a management scheme for electric vehicle charging, considering the massive penetration of these can cause negative effects on distribution networks, compromising the reliability, quality and security of system. With the proposed algorithm, the network operator will benefit by avoiding the overload of distribution circuit, minimizing the power losses and improving the voltage profile. The proposed model assigns an initial charge for each vehicle following a probability function that represents the required energy based on mobility patterns of the city, the capacity and discharged energy of battery. Finally, we verified the effectiveness of the proposed management scheme to analyzing a study case for the city of Bogotá., Este artículo presenta un esquema de gestión para la recarga de vehículos eléctricos, considerando que la penetración masiva de estos puede generar efectos negativos en las redes de distribución, comprometiendo la confiabilidad, calidad y seguridad del sistema. Con el algoritmo propuesto, el operador de red se beneficia al evitar la sobrecarga del circuito de distribución, reducir las pérdidas de potencia y mejorar el perfil de tensión. El modelo planteado asigna una carga inicial a cada vehículo siguiendo una función de probabilidad que representa la energía requerida según los patrones de movilidad de la ciudad, la capacidad de la batería y el consumo. Finalmente, se comprueba la efectividad del esquema de gestión propuesto analizando un caso de estudio para la ciudad de Bogotá.
Published: 2015

35. Algoritmo de gestión para la recarga de vehículos eléctricos

Author: Mendoza, C, Quintero, A, Alarcón, J, Mendoza, C, Quintero, A, and Alarcón, J
Abstract: This article presents a management scheme for electric vehicle charging, considering the massive penetration of these can cause negative effects on distribution networks, compromising the reliability, quality and security of system. With the proposed algorithm, the network operator will benefit by avoiding the overload of distribution circuit, minimizing the power losses and improving the voltage profile. The proposed model assigns an initial charge for each vehicle following a probability function that represents the required energy based on mobility patterns of the city, the capacity and discharged energy of battery. Finally, we verified the effectiveness of the proposed management scheme to analyzing a study case for the city of Bogotá., Este artículo presenta un esquema de gestión para la recarga de vehículos eléctricos, considerando que la penetración masiva de estos puede generar efectos negativos en las redes de distribución, comprometiendo la confiabilidad, calidad y seguridad del sistema. Con el algoritmo propuesto, el operador de red se beneficia al evitar la sobrecarga del circuito de distribución, reducir las pérdidas de potencia y mejorar el perfil de tensión. El modelo planteado asigna una carga inicial a cada vehículo siguiendo una función de probabilidad que representa la energía requerida según los patrones de movilidad de la ciudad, la capacidad de la batería y el consumo. Finalmente, se comprueba la efectividad del esquema de gestión propuesto analizando un caso de estudio para la ciudad de Bogotá.
Published: 2015

36. Monitoring and management of Pyrenean chamois in Aragon

Author: Herrero Cortés, Juan, Alarcón, J. L., Escudero, Emilio, Fernández-Arberas, Olatz, García-González, Ricardo, García Serrano, Alicia, Herrero Cortés, Juan, Alarcón, J. L., Escudero, Emilio, Fernández-Arberas, Olatz, García-González, Ricardo, and García Serrano, Alicia
Published: 2015

37. The role of the $\Delta(1232)$-resonance in covariant baryon chiral perturbation theory

Author: Alarcón, J. M. and Alarcón, J. M.
Abstract: We stress, on theoretical and phenomenological grounds, the importance of the $\Delta(1232)$-resonance in a chiral effective field theory approach applied to the study of $\pi N$ scattering. We show how its inclusion as a dynamical degree of freedom allow us to obtain reliably valuable information from $\pi N$ scattering data., Comment: Contribution to NSTAR 2013, May 27-30, 2013, Peniscola (Spain); 4 pages
Published: 2013
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38. Low energy analysis of $\pi N$ scattering and the pion-nucleon sigma term with covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: The pion-nucleon sigma term ($\sigma_{\pi N}$) is an observable of fundamental importance because embodies information about the internal scalar structure of the nucleon. Nowadays this quantity has triggered renewed interest because it is a key input for a reliable estimation of the dark matter-nucleon spin independent elastic scattering cross section. In this proceeding we present how this quantity can be reliably extracted by employing only experimental information with the use covariant baryon chiral perturbation theory. We also contrast our extraction with updated phenomenology related to $\sigma_{\pi N}$ and show how this phenomenology favours a relatively large value of $\sigma_{\pi N}$. Finally, we extract a value of $\sigma_{\pi N}=59(7)$ MeV from modern partial wave analyses data., Comment: PROCEEDINGS to Xth "Quark Confinement and the Hadron Spectrum"- 8 Pag,, 4 Tables, 2 Figures. TUM Campus Garching, Munich, Germany: October 8-12, 2012. Version 2: 2 references added
Published: 2013

39. The role of the $\Delta(1232)$-resonance in covariant baryon chiral perturbation theory

Author: Alarcón, J. M. and Alarcón, J. M.
Abstract: We stress, on theoretical and phenomenological grounds, the importance of the $\Delta(1232)$-resonance in a chiral effective field theory approach applied to the study of $\pi N$ scattering. We show how its inclusion as a dynamical degree of freedom allow us to obtain reliably valuable information from $\pi N$ scattering data., Comment: Contribution to NSTAR 2013, May 27-30, 2013, Peniscola (Spain); 4 pages
Published: 2013
Full Text: View/download PDF

40. Low energy analysis of $\pi N$ scattering and the pion-nucleon sigma term with covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: The pion-nucleon sigma term ($\sigma_{\pi N}$) is an observable of fundamental importance because embodies information about the internal scalar structure of the nucleon. Nowadays this quantity has triggered renewed interest because it is a key input for a reliable estimation of the dark matter-nucleon spin independent elastic scattering cross section. In this proceeding we present how this quantity can be reliably extracted by employing only experimental information with the use covariant baryon chiral perturbation theory. We also contrast our extraction with updated phenomenology related to $\sigma_{\pi N}$ and show how this phenomenology favours a relatively large value of $\sigma_{\pi N}$. Finally, we extract a value of $\sigma_{\pi N}=59(7)$ MeV from modern partial wave analyses data., Comment: PROCEEDINGS to Xth "Quark Confinement and the Hadron Spectrum"- 8 Pag,, 4 Tables, 2 Figures. TUM Campus Garching, Munich, Germany: October 8-12, 2012. Version 2: 2 references added
Published: 2013

41. Low energy analysis of $\pi N$ scattering and the pion-nucleon sigma term with covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: The pion-nucleon sigma term ($\sigma_{\pi N}$) is an observable of fundamental importance because embodies information about the internal scalar structure of the nucleon. Nowadays this quantity has triggered renewed interest because it is a key input for a reliable estimation of the dark matter-nucleon spin independent elastic scattering cross section. In this proceeding we present how this quantity can be reliably extracted by employing only experimental information with the use covariant baryon chiral perturbation theory. We also contrast our extraction with updated phenomenology related to $\sigma_{\pi N}$ and show how this phenomenology favours a relatively large value of $\sigma_{\pi N}$. Finally, we extract a value of $\sigma_{\pi N}=59(7)$ MeV from modern partial wave analyses data., Comment: PROCEEDINGS to Xth "Quark Confinement and the Hadron Spectrum"- 8 Pag,, 4 Tables, 2 Figures. TUM Campus Garching, Munich, Germany: October 8-12, 2012. Version 2: 2 references added
Published: 2013

42. Improved description of the $\pi N$-scattering phenomenology in covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: We present a novel analysis of the $\pi N$ scattering amplitude in covariant baryon chiral perturbation theory up to ${\cal O}(p^3)$ within the extended-on-mass-shell renormalization scheme and including the $\Delta(1232)$ explicitly in the $\delta$-counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the $\pi N$ scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger-Treiman relation, the pion-nucleon sigma term and the extrapolation onto the subthreshold region. The chiral representation of the amplitude in the theory with the $\Delta$ presents a good convergence from very low energies in the subthreshold region up to energies well above threshold, leading also to a phenomenological description perfectly consistent with the one reported by the respective partial wave analyses and independent determinations. We conclude that a model-independent and systematic framework to analyze $\pi N$-scattering observables using directly experimental data shall be possible in covariant baryon chiral perturbation theory., Comment: 64 pages, 19 figures, 18 tables
Published: 2012
Full Text: View/download PDF

43. Improved description of the $\pi N$-scattering phenomenology in covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: We present a novel analysis of the $\pi N$ scattering amplitude in covariant baryon chiral perturbation theory up to ${\cal O}(p^3)$ within the extended-on-mass-shell renormalization scheme and including the $\Delta(1232)$ explicitly in the $\delta$-counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the $\pi N$ scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger-Treiman relation, the pion-nucleon sigma term and the extrapolation onto the subthreshold region. The chiral representation of the amplitude in the theory with the $\Delta$ presents a good convergence from very low energies in the subthreshold region up to energies well above threshold, leading also to a phenomenological description perfectly consistent with the one reported by the respective partial wave analyses and independent determinations. We conclude that a model-independent and systematic framework to analyze $\pi N$-scattering observables using directly experimental data shall be possible in covariant baryon chiral perturbation theory., Comment: 64 pages, 19 figures, 18 tables
Published: 2012
Full Text: View/download PDF

44. Improved description of the $\pi N$-scattering phenomenology in covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: We present a novel analysis of the $\pi N$ scattering amplitude in covariant baryon chiral perturbation theory up to ${\cal O}(p^3)$ within the extended-on-mass-shell renormalization scheme and including the $\Delta(1232)$ explicitly in the $\delta$-counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the $\pi N$ scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger-Treiman relation, the pion-nucleon sigma term and the extrapolation onto the subthreshold region. The chiral representation of the amplitude in the theory with the $\Delta$ presents a good convergence from very low energies in the subthreshold region up to energies well above threshold, leading also to a phenomenological description perfectly consistent with the one reported by the respective partial wave analyses and independent determinations. We conclude that a model-independent and systematic framework to analyze $\pi N$-scattering observables using directly experimental data shall be possible in covariant baryon chiral perturbation theory., Comment: 64 pages, 19 figures, 18 tables
Published: 2012
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45. Improved description of the $\pi N$-scattering phenomenology in covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: We present a novel analysis of the $\pi N$ scattering amplitude in covariant baryon chiral perturbation theory up to ${\cal O}(p^3)$ within the extended-on-mass-shell renormalization scheme and including the $\Delta(1232)$ explicitly in the $\delta$-counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the $\pi N$ scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger-Treiman relation, the pion-nucleon sigma term and the extrapolation onto the subthreshold region. The chiral representation of the amplitude in the theory with the $\Delta$ presents a good convergence from very low energies in the subthreshold region up to energies well above threshold, leading also to a phenomenological description perfectly consistent with the one reported by the respective partial wave analyses and independent determinations. We conclude that a model-independent and systematic framework to analyze $\pi N$-scattering observables using directly experimental data shall be possible in covariant baryon chiral perturbation theory., Comment: 64 pages, 19 figures, 18 tables
Published: 2012
Full Text: View/download PDF

46. Improved description of the $\pi N$-scattering phenomenology in covariant baryon chiral perturbation theory

Author: Alarcón, J. M., Camalich, J. Martin, Oller, J. A., Alarcón, J. M., Camalich, J. Martin, and Oller, J. A.
Abstract: We present a novel analysis of the $\pi N$ scattering amplitude in covariant baryon chiral perturbation theory up to ${\cal O}(p^3)$ within the extended-on-mass-shell renormalization scheme and including the $\Delta(1232)$ explicitly in the $\delta$-counting. We take the hadronic phase shifts provided by partial wave analyses as basic experimental information to fix the low-energy constants. Subsequently, we study in detail the various observables and low-energy theorems related to the $\pi N$ scattering amplitude. In particular, we discuss the results and chiral expansion of the phase shifts, the threshold coefficients, the Goldberger-Treiman relation, the pion-nucleon sigma term and the extrapolation onto the subthreshold region. The chiral representation of the amplitude in the theory with the $\Delta$ presents a good convergence from very low energies in the subthreshold region up to energies well above threshold, leading also to a phenomenological description perfectly consistent with the one reported by the respective partial wave analyses and independent determinations. We conclude that a model-independent and systematic framework to analyze $\pi N$-scattering observables using directly experimental data shall be possible in covariant baryon chiral perturbation theory., Comment: 64 pages, 19 figures, 18 tables
Published: 2012
Full Text: View/download PDF

47. Relativistic chiral representation of the \pi N scattering amplitude

Author: Alarcón, J. M., Camalich, J. Martín, Oller, J. A., Alvarez-Ruso, L., Alarcón, J. M., Camalich, J. Martín, Oller, J. A., and Alvarez-Ruso, L.
Abstract: We have analyzed pion-nucleon scattering using the manifestly relativistic covariant frameworks of Infrared Regularization (IR) and Extended-On-Mass-Shell (EOMS) up to O(q^3) in the chiral expansion, where q is a generic small momentum. We describe the low-energy phase shifts with a similar quality as previously achieved with Heavy Baryon Chiral Perturbation Theory, being the EOMS description better than the IR one. The Goldberger-Treiman discrepancy is extracted from data of partial wave analyses using both schemes, obtaining an unacceptable large value for the case of IR due to the loop contribution. On the other hand, EOMS gives small values compatible with other phenomenological approaches. Finally, we have unitarized the amplitudes provided by both schemes to extend the range of our description obtaining a good agreement with the data up to energies of \sqrt{s}\approx 1.3 GeV for the EOMS scheme while IR can not go beyond energies of \sqrt{s}\approx 1.25 GeV due to the unphysical cut that this scheme introduces., Comment: 6 pages, 2 figures. Proceeding of XIV International Conference on Hadron Spectroscopy (hadron2011). A shorter version of this work was also presented in the 8th International Workshop on the Physics of Excited Nucleons (NSTAR 2011)
Published: 2011

48. Devising irrigation water tariffs with overconsumption penalties

Author: Mesa Jurado, M. A., Berbel, Julio, Alarcón, J., Mesa Jurado, M. A., Berbel, Julio, and Alarcón, J.
Abstract: The paper analyses an irrigation water tariff model to control overconsumption by implementing effective penalties that can be seen as a supplementary tool to crop-specific quotas. This progressive pricing system is based on the financial loss that farmers would face when having to reduce their irrigation water consumption in order to comply with the commitment to achieving more restrictive quotas. Results show that a single fixed price system (with a flat rate) is costlier to farmers than the differentiated tariff system, which distinguishes the amount of water that exceeds the established allocation from the quantity below. This system of irrigation water pricing and overconsumption penalties, aimed specifically at each crop, facilitates efficient utilisation and the ability to adjust this consumption to resource availability and current economic and market situations, especially in response to crop subsidies. The practical barriers to implementing differentiated tariffs per crop with overconsumption penalties are the availability of irrigation water marginal productivity and net profit functions, and having to install technological equipment to control the water being used by individual farmers.
Published: 2011

49. Relativistic chiral representation of the \pi N scattering amplitude

Author: Alarcón, J. M., Camalich, J. Martín, Oller, J. A., Alvarez-Ruso, L., Alarcón, J. M., Camalich, J. Martín, Oller, J. A., and Alvarez-Ruso, L.
Abstract: We have analyzed pion-nucleon scattering using the manifestly relativistic covariant frameworks of Infrared Regularization (IR) and Extended-On-Mass-Shell (EOMS) up to O(q^3) in the chiral expansion, where q is a generic small momentum. We describe the low-energy phase shifts with a similar quality as previously achieved with Heavy Baryon Chiral Perturbation Theory, being the EOMS description better than the IR one. The Goldberger-Treiman discrepancy is extracted from data of partial wave analyses using both schemes, obtaining an unacceptable large value for the case of IR due to the loop contribution. On the other hand, EOMS gives small values compatible with other phenomenological approaches. Finally, we have unitarized the amplitudes provided by both schemes to extend the range of our description obtaining a good agreement with the data up to energies of \sqrt{s}\approx 1.3 GeV for the EOMS scheme while IR can not go beyond energies of \sqrt{s}\approx 1.25 GeV due to the unphysical cut that this scheme introduces., Comment: 6 pages, 2 figures. Proceeding of XIV International Conference on Hadron Spectroscopy (hadron2011). A shorter version of this work was also presented in the 8th International Workshop on the Physics of Excited Nucleons (NSTAR 2011)
Published: 2011

50. CYFRA 21-1 as a tool for distant metastasis detection in lung cancer

Author: Cabrera-Alarcón, J. L, Carrillo-Vico, Antonio, Santotoribio, José D., León-Justel, Antonio, Sánchez-Gil, R., González-Castro, A., Guerrero Montávez, Juan Miguel, Cabrera-Alarcón, J. L, Carrillo-Vico, Antonio, Santotoribio, José D., León-Justel, Antonio, Sánchez-Gil, R., González-Castro, A., and Guerrero Montávez, Juan Miguel
Abstract: [Background] A study to analyse tumor markers (CEA, CA125, CA15.3, CA19.9, CYFRA 21-1, and NSE) for metastasis detection in lung cancer patients., [Methods] Serum tumor markers from 73 lung cancer patients were measured before they were diagnosed. After lung cancer diagnosis, tumor markers were analyzed for the detection of distant metastases., [Results] In NSCLC patients CYFRA 21-1 and NSE showed differences between stage IV and any of the other stages, p <0.05. The accuracy for metastasis detection was AUC = 81.5% for CYFRA 21-1 and AUC = 78.6% for NSE. CYFRA 21-1 (OR = 1.406; 95% CI, 1.087 - 1.821, p <0.01) and NSE (OR = 1.197; 95% CI, 1.011 - 1.416, p <0.05) were independent predictors for metastasis presence. No tumor marker showed significant differences according to stages in SCLC patients., [Conclusions] CYFRA 21-1 could be used as a screening tool for metastasis detection in lung cancer patients without symptoms of metastasis as well as CYFRA 21-1 and NSE in NSCLC patients.
Published: 2011

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