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413 results on '"Henson, B"'

1. Trap Frequency Measurement with a Pulsed Atom Laser

Author

Henson, B. M., Thomas, K. F., Mehdi, Z., Burnett, T. G., Ross, J. A., Hodgman, S. S., and Truscott, A. G.

Subjects
Condensed Matter - Quantum Gases
Abstract

We describe a novel method of single-shot trap frequency measurement for a confined Bose-Einstein Condensate, which uses an atom laser to repeatedly sample the mean velocity of trap oscillations as a function of time. The method is able to determine the trap frequency to an accuracy of 39~ppm (16~mHz) in a single experimental realization, improving on the literature by a factor of three. Further, we show that by employing a reconstructive aliasing approach our method can be applied to trap frequencies more than a factor of 3 greater than the sampling frequency., Comment: 13 pages, 6 figures, removed ~ in abstract

Published
2022
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2. Measurement of a helium tune-out frequency: an independent test of quantum electrodynamics

Author

Henson, B. M., Ross, J. A., Thomas, K. F., Kuhn, C. N., Shin, D. K., Hodgman, S. S., Zhang, Yong-Hui, Tang, Li-Yan, Drake, G. W. F., Bondy, A. T., Truscott, A. G., and Baldwin, K. G. H.

Subjects
Physics - Atomic Physics, Condensed Matter - Quantum Gases
Abstract

Despite quantum electrodynamics (QED) being one of the most stringently tested theories underpinning modern physics, recent precision atomic spectroscopy measurements have uncovered several small discrepancies between experiment and theory. One particularly powerful experimental observable that tests QED independently of traditional energy level measurements is the `tune-out' frequency, where the dynamic polarizability vanishes and the atom does not interact with applied laser light. In this work, we measure the `tune-out' frequency for the $2^{3\!}S_1$ state of helium between transitions to the $2^{3\!}P$ and $3^{3\!}P$ manifolds and compare it to new theoretical QED calculations. The experimentally determined value of $725\,736\,700\,$$(40_{\mathrm{stat}},260_{\mathrm{syst}})$ MHz is within ${\sim} 1.7\sigma$ of theory ($725\,736\,252(9)$ MHz), and importantly resolves both the QED contributions (${\sim} 30 \sigma$) and novel retardation (${\sim} 2 \sigma$) corrections., Comment: Main text 6 pages, 4 figures, SI 21 pages 11 figures. Changed title from "Precision Measurement of the Helium $2^{3\!}S_1- 2^{3\!}P/3^{3\!}P$ Tune-Out Frequency as a Test of QED"

Published
2021
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3. On the survival of the quantum depletion of a condensate after release from a magnetic trap

Author

Ross, J. A., Deuar, P., Shin, D. K., Thomas, K. F., Henson, B. M., Hodgman, S. S., and Truscott, A. G.

Subjects
Condensed Matter - Quantum Gases
Abstract

We present observations of the high momentum tail in expanding Bose-Einstein condensates of metastable Helium atoms released from a harmonic trap. The far-field density profile exhibits features that support identification of the tails of the momentum distribution as originating in the in-situ quantum depletion prior to release. Thus, we corroborate recent observations of slowly-decaying tails in the far-field beyond the thermal component. This observation is in conflict with the hydrodynamic theory, which predicts that the in-situ depletion does not survive when atoms are released from a trap. Indeed, the depleted tails even appear stronger in the far-field than expected before release, and we discuss the challenges of interpreting this in terms of the Tan contact in the trapped gas. In complement to these observations, full quantum simulations of the experiment show that, under the right conditions, the depletion can persist into the far field after expansion. Moreover, the simulations provide mechanisms for survival and for the the large-momentum tails to appear stronger after expansion due to an acceleration of the depleted atoms by the mean-field potential. However, while in qualitative agreement, the final depletion observed in the experiment is much larger than in the simulation., Comment: 17 pages, 9 figures

Published
2021
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4. Direct Measurement of the Forbidden $2^{3\!}S_1 \rightarrow 3^{3\!}S_1$ Atomic Transition in Helium

Author

Thomas, K. F., Ross, J. A., Henson, B. M., Shin, D. K., Baldwin, K. G. H., Hodgman, S. S., and Truscott, A. G.

Subjects
Physics - Atomic Physics
Abstract

We present the detection of the highly forbidden $2^{3\!}S_1 \rightarrow 3^{3\!}S_1$ atomic transition in helium, the weakest transition observed in any neutral atom. Our measurements of the transition frequency, upper state lifetime, and transition strength agree well with published theoretical values, and can lead to tests of both QED contributions and different QED frameworks. To measure such a weak transition, we developed two methods using ultracold metastable ($2^{3\!}S_1$) helium atoms: low background direct detection of excited then decayed atoms for sensitive measurement of the transition frequency and lifetime; and a pulsed atom laser heating measurement for determining the transition strength. These methods could possibly be applied to other atoms, providing new tools in the search for ultra-weak transitions and precision metrology., Comment: 18 pages, 13 figures, 3 tables

Published
2020
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5. Entanglement-based 3D magnetic gradiometry with an ultracold atomic scattering halo

Author

Shin, D. K., Ross, J. A., Henson, B. M., Hodgman, S. S., and Truscott, A. G.

Subjects
Quantum Physics
Abstract

Ultracold collisions of Bose-Einstein condensates can be used to generate a large number of counterpropagating pairs of entangled atoms, which collectively form a thin spherical shell in momentum space, called a scattering halo. Here we generate a scattering halo composed almost entirely of pairs in a symmetric entangled state and observe a scattering angle-dependent mixing to the anti-symmetric state due to the presence of an inhomogeneous magnetic field. We report on a proof-of-principle application of the observed parity dynamics to demonstrate magnetic gradiometry, insensitive to common-mode fluctuations of the background magnetic field. Furthermore, the highly multimode nature and narrow radial width of the scattering halos enable 3D tomography of an interrogated field without the need for a scanning probe., Comment: 13 pages, 9 figures

Published
2019
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6. A strong Bell correlation witness between spatially separated pairs of atoms

Author

Shin, D. K., Henson, B. M., Hodgman, S. S., Wasak, T., Chwedenczuk, J., and Truscott, A. G.

Subjects
Quantum Physics, Condensed Matter - Quantum Gases
Abstract

The violation of a Bell inequality is a striking demonstration of how quantum mechanics contradicts local realism. Although the original argument was presented with a pair of spin 1/2 particles, so far Bell inequalities have been shown to be violated using entangled pairs of photons, with recent measurements closing all possible loopholes in such a scheme. Equivalent demonstrations using massive particles have proven to be much more challenging, generally relying on post-selection of data or measuring an entanglement witness that relies on quantum mechanics. Here, we use a collision between two Bose-Einstein condensates to generate the momentum-spin entangled pairs of ultracold helium atoms. We show that a maximally entangled Bell triplet state results and report a direct observation of a strong Bell correlation witness. Based on the high degree of entanglement and the controllability of ultracold atomic systems, extensions to this scheme would allow a demonstration of nonlocality with massive entangled pairs, following the original idea of Bell. Other applications include the demonstration of the Einstein-Podolsky-Rosen paradox, quantum metrology and tests of phenomena from exotic theories sensitive to such systems including gravitational decoherence and quantum gravity.

Published
2018
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7. Bogoliubov-Cherenkov Radiation in an Atom Laser

Author

Henson, B. M., Yue, Xuguang, Hodgman, S. S., Shin, D. K., Smirnov, L. A., Ostrovskaya, E. A., Guan, X. W., and Truscott, A. G.

Subjects
Condensed Matter - Quantum Gases, Nonlinear Sciences - Pattern Formation and Solitons
Abstract

We develop a simple yet powerful technique to study Bogoliubov-Cherenkov radiation by producing a pulsed atom laser from a strongly confined Bose-Einstein condensate. Such radiation results when the atom laser pulse falls past a Bose-Einstein condensate at high-hypersonic speeds, modifying the spatial profile to display a characteristic twin jet structure and a complicated interference pattern. The experimental observations are in excellent agreement with mean-field numerical simulations and an analytic theory. Due to the highly hypersonic regime reached in our experiment, this system offers a highly controllable platform for future studies of condensed-matter analogs of quantum electrodynamics at ultrarelativistic speeds., Comment: 14 pages 9 figures. v4 changes: \v{C}herenkov changed to Cherenkov

Published
2017
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9. The First Measurement of the $2^{3\!}S_1 - 2^{3\!}P / 3^{3\!}P$ Tune-Out Wavelength in He*

Author

Henson, B. M.

Subjects
Physics - Atomic Physics, Physics - Optics, 81V45
Abstract

The workhorse of atomic physics, quantum electrodynamics, is one of the best-tested theories in physics. However recent discrepancies have shed doubt on its accuracy for complex atomic systems. To facilitate the development of the theory further we aim to measure transition dipole matrix elements of metastable helium (He*) (the ideal 3 body test-bed) to the highest accuracy thus far. We have undertaken a measurement of the `tune-out wavelength' which occurs when the contributions to the dynamic polarizability from all atomic transitions sum to zero; thus illuminating an atom with this wavelength of light then produces no net energy shift. This provides a strict constraint on the transition dipole matrix elements without the complication and inaccuracy of other methods. Using a novel atom-laser based technique we have made the first measurement of the tune-out wavelength in metastable helium between the $3^{3}P_{1,2,3}$ and $2^{3}P_{1,2,3}$ states at 413.07(2) nm which compares well with the predicted value [PhysRevA.88.052515] of 413.02(9) nm. We have additionally developed many of the methods necessary to improve this measurement to the 100 fm level of accuracy where it will form the most accurate determination of transition rate information ever made in He* and provide a stringent test for atomic QED simulations. We believe this measurement to be one of the most sensitive ever made of an optical dipole potential, able to detect changes in potentials of $\sim$200 pK and is widely applicable to other species and areas of atom optics., Comment: Citation note added. Corrected typo. References changed to biblatex

Published
2017

10. Ghost Imaging with Atoms

Author

Khakimov, R. I., Henson, B. M., Shin, D. K., Hodgman, S. S., Dall, R. G., Baldwin, K. G. H., and Truscott, A. G.

Subjects
Condensed Matter - Quantum Gases, Physics - Atomic Physics, Physics - Optics, Quantum Physics
Abstract

Ghost imaging is a technique -- first realized in quantum optics -- in which the image emerges from cross-correlation between particles in two separate beams. One beam passes through the object to a bucket (single-pixel) detector, while the second beam's spatial profile is measured by a high resolution (multi-pixel) detector but never interacts with the object. Neither detector can reconstruct the image independently. However, until now ghost imaging has only been demonstrated with photons. Here we report the first realisation of ghost imaging of an object using massive particles. In our experiment, the two beams are formed by correlated pairs of ultracold metastable helium atoms, originating from two colliding Bose-Einstein condensates (BECs) via $s$-wave scattering. We use the higher-order Kapitza-Dirac effect to generate the large number of correlated atom pairs required, enabling the creation of a ghost image with good visibility and sub-millimetre resolution. Future extensions could include ghost interference as well as tests of EPR entantlement and Bell's inequalities.

Published
2016
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11. Precision Measurement for Metastable Helium Atoms of the 413 nm Tune-Out Wavelength at Which the Atomic Polarizability Vanishes

Author

Henson, B. M., Khakimov, R. I., Dall, R. G., Baldwin, K. G. H., Tang, Li-Yan, and Truscott, A. G.

Subjects
Physics - Atomic Physics
Abstract

We present the first measurement for helium atoms of the tune-out wavelength at which the atomic polarizability vanishes. We utilise a novel, highly sensitive technique for precisely measuring the effect of variations in the trapping potential of confined metastable ($2^{3}S_{1}$) helium atoms illuminated by a perturbing laser light field. The measured tune-out wavelength of 413.0938($9_{Stat.}$)($20_{Syst.}$) nm compares well with the value predicted by a theoretical calculation (413.02(9) nm) which is sensitive to finite nuclear mass, relativistic, and quantum electro-dynamic (QED) effects. This provides motivation for more detailed theoretical investigations to test QED., Comment: 5 pages, 4 figures

Published
2015
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12. Applications of chemical kinetics to detonation: Wave coalescence and homogeneous initiation in single crystal 1,3-propanediol-2,2-bis[(nitrooxy)methyl]-tetranitrate (PETN).

Author

Henson, B. F. and Smilowitz, L.

Abstract

A thermal ignition model is used in parallel with single crystal solid and product fluid Equations of State (EOSs) from the literature to calculate the time and distance to homogeneous shock initiation in single crystal 1,3-propanediol-2,2-bis[(nitrooxy)methyl]-tetranitrate (PETN). The ignition model is a highly constrained, globalized representation of the temperature and pressure dependent decomposition chemistry of PETN. Initiation in the single crystal proceeds via a homogeneous initiation mechanism where thermal ignition results from a well defined initial shock state (P,V,T). The transition to steady detonation at an observed location (x*, t*) then follows when a superdetonation wave initiated by this thermal ignition overtakes the input shock wave. In the traditional approach, P and V are determined directly from measurements and conservation of mass and momentum, leaving T relatively unconstrained due to the extremely nonlinear dependence of T on P, V in the EOS. We present an iterative algorithm to calculate T and V as a function of P from the time to thermal ignition, superdetonation, and intersection at (x*, t*) observed in each experiment. These states are consistent with the unreacted EOS but allow an independent determination of the energy deposited into heating by the input shock. The calculated states compare favorably with pressures and states of compression observed in the experiment but provide a new and interesting set of temperatures associated with each state. We discuss these fully determined initial shock states in (P, V, T) in the context of PETN thermodynamics, specifically the solid/liquid phase boundary at high temperature and pressure. [ABSTRACT FROM AUTHOR]

Published
2022
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13. A scoping review of current and emerging techniques for evaluation of peripheral nerve health, degeneration and regeneration: part 2, non-invasive imaging

Author

Mandeville, Ross, primary, Deshmukh, Swati, additional, Tan, Ek Tsoon, additional, Kumar, Viksit, additional, Sanchez, Benjamin, additional, Dowlatshahi, Arriyan S, additional, Luk, Justin, additional, See, Reiner Henson B, additional, Leochico, Carl Froilan D, additional, Thum, Jasmine A, additional, Bazarek, Stanley, additional, Johnston, Benjamin, additional, Brown, Justin, additional, Wu, Jim, additional, Sneag, Darryl, additional, and Rutkove, Seward, additional

Published
2023
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14. A scoping review of current and emerging techniques for evaluation of peripheral nerve health, degeneration, and regeneration: part 1, neurophysiology

Author

Mandeville, Ross, primary, Sanchez, Benjamin, additional, Johnston, Benjamin, additional, Bazarek, Stanley, additional, Thum, Jasmine A, additional, Birmingham, Austin, additional, See, Reiner Henson B, additional, Leochico, Carl Froilan D, additional, Kumar, Viksit, additional, Dowlatshahi, Arriyan S, additional, Brown, Justin, additional, Stashuk, Daniel, additional, and Rutkove, Seward B, additional

Published
2023
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17. Experimental observations of exploding bridgewire detonator function.

Author

Smilowitz, L., Henson, B. F., Remelius, D., Bowlan, P., Suvorova, N., Allison, J., Cardon, D., Freeman, M., Mariam, F., Meijer, W., Morris, C., Neukirch, L., Prestridge, K., Sandstrom, M., Saunders, A., Schurman, T., Tainter, A., Tang, Z., Trouw, F., and Tupa, D.

Subjects
*DETONATORS, *DETONATION waves, *X-rays, *VISIBLE spectra, *YEAR, *TEMPERATURE measurements
Abstract

Exploding bridgewire detonators are an industry standard technology used for over 75 years and valued for their precise timing and safety characteristics. Despite widespread use, their functional mechanism remains controversial with both shock and non-shock mechanisms attributed. In this work, we reexamine the bridgewire detonator function with a suite of modern diagnostics and compare these observations with the existing literature. Traditional detonator observations consisted of voltage applied to the bridgewire and time dependent current, integral response measurements such as case motion, and more recently Schlieren imaging of the detonator surface. In this work, we add visible light emission, x-ray transmission, proton radiography, and temperature measurements during detonator function in addition to voltage, current, and function times. The addition of in situ observations of light emission, temperature, and density gives us new insight into the mechanisms of explosive bridgewire detonator function. We see a distinct separation in time, location, symmetry, and velocity of bridgewire output and detonation onset. During the time between bridgewire burst and the initiation of detonation, we observe a temperature ramp in the input pellet. In this paper, we present the suite of measurements and comparisons with the literature on integral response measurements. [ABSTRACT FROM AUTHOR]

Published
2020
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21. Kinetics of the γ–δ phase transition in energetic nitramine-octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine.

Author

Bowlan, P., Henson, B. F., Smilowitz, L., Levitas, V. I., Suvorova, N., and Oschwald, D.

Subjects
*PHASE transitions, *MELTING points, *TRANSITION temperature, *DISCONTINUOUS precipitation, *NUCLEATION, *MOLECULAR conformation
Abstract

The solid, secondary explosive nitramine-octahydro-1,3,5,7-tetranitro-1,3,5,7 or HMX has four different stable polymorphs which have different molecular conformations, crystalline structures, and densities, making structural phase transitions between these nontrivial. Previous studies of the kinetics of the β–δ HMX structural transition found this to happen by a nucleation and growth mechanism, where growth was governed by the heat of fusion, or melting, even though the phase transition temperature is more than 100 K below the melting point. A theory known as virtual melting could easily justify this since the large volume difference in the two phases creates a strain at their interface that can lower the melting point to the phase transition temperature through a relaxation of the elastic energy. To learn more about structural phase transitions in organic crystalline solids and virtual melting, here we use time-resolved X-ray diffraction to study another structural phase transition in HMX, γ–δ. Again, second order kinetics are observed which fit to the same nucleation and growth model associated with growth by melting even though the volume change in this transition is too small to lower the melting point by interfacial strain. To account for this, we present a more general model illustrating that melting over a very thin layer at the interface between the two phases reduces the total interfacial energy and is therefore thermodynamically favorable and can drive the structural phase transition in the absence of large volume changes. Our work supports the idea that virtual melting may be a more generally applicable mechanism for structural phase transitions in organic crystalline solids. [ABSTRACT FROM AUTHOR]

Published
2019
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24. Index

Author

Henson, Bryce

Published
2024

25. Cover

Author

Henson, Bryce

Published
2024

30. Notes

Author

Henson, Bryce

Published
2024

50. Effect of lorcaserin on prevention and remission of type 2 diabetes in overweight and obese patients (CAMELLIA-TIMI 61): a randomised, placebo-controlled trial

Author

Bohula, Erin A, primary, Scirica, Benjamin M, additional, Inzucchi, Silvio E, additional, McGuire, Darren K, additional, Keech, Anthony C, additional, Smith, Steven R, additional, Kanevsky, Estella, additional, Murphy, Sabina A, additional, Leiter, Lawrence A, additional, Dwyer, Jamie P, additional, Corbalan, Ramon, additional, Hamm, Christian, additional, Kaplan, Lee, additional, Nicolau, Jose Carlos, additional, Ophuis, Ton Oude, additional, Ray, Kausik K, additional, Ruda, Mikhail, additional, Spinar, Jindrich, additional, Patel, Tushar, additional, Miao, Wenfeng, additional, Perdomo, Carlos, additional, Francis, Bruce, additional, Dhadda, Shobha, additional, Bonaca, Marc P, additional, Ruff, Christian T, additional, Sabatine, Marc S, additional, Wiviott, Stephen D, additional, Inzucchi, Silvio, additional, Keech, Anthony, additional, Satlin, Andrew, additional, Brown, Conville, additional, Budaj, Andrzej, additional, Dwyer, Jamie, additional, Garcia-Castillo, Armando, additional, Gupta, Milan, additional, Oude Ophuis, Ton, additional, Ray, Kauski, additional, Weissman, Neil, additional, White, Harvey D, additional, Amerena, J, additional, Arstall, M, additional, Colquhoun, D, additional, Jayasinghe, R, additional, Lee, A, additional, Lehman, R, additional, Moses, R, additional, Proietto, J, additional, Purnell, P, additional, Waites, J, additional, Blombery, P, additional, Cross, D, additional, Worthley, M, additional, d'Emden, M, additional, Selvanayagam, J, additional, Oqueli, RE, additional, Whelan, A, additional, Garrahy, P, additional, de Looze, F, additional, Ninio, D, additional, Horowitz, J, additional, William, M, additional, Suranyi, M, additional, Wittert, G, additional, Le May, M, additional, Pandey, AS, additional, Vizel, S, additional, Labonte, R, additional, Beaudry, Y, additional, Fortin, C, additional, Bell, A, additional, Kouz, S, additional, St-Amour, É, additional, Bata, I, additional, St Maurice, F, additional, Chehayeb, R, additional, Constance, C, additional, Wong, G, additional, Hess, A, additional, Liutkus, J, additional, Poirier, P, additional, Teitelbaum, I, additional, Berlingieri, J, additional, Cha, J, additional, Hartleib, M, additional, Heffernan, M, additional, Twum-Barima, D, additional, Pandith, V, additional, Aronson, R, additional, Goldenberg, R, additional, Ajala, B, additional, Jain, A, additional, Ross, S, additional, Bajaj, H, additional, Khandwala, H, additional, Yared, Z, additional, Gupta, N, additional, Bédard, J, additional, Wharton, S, additional, Blouin, F, additional, Savard, D, additional, Shukla, D, additional, Cobos, J, additional, Godoy, G, additional, Perez, L, additional, Pincetti, C, additional, Saavedra Guajardo, V, additional, Varleta, P, additional, Conejeros, C, additional, Lanas, F, additional, Bayram Llamas, E, additional, Cardona Muñoz, E, additional, Garcia, R, additional, Garza Ruiz, J, additional, Llamas Esperon, G, additional, Lopez Rosas, E, additional, Melendez Mier, G, additional, Ramos, G, additional, Hart, H, additional, Scott, D, additional, Ternouth, I, additional, Benatar, J, additional, Elliott, J, additional, Cutfield, R, additional, Manning, P, additional, Williams, M, additional, Ferrier, K, additional, Scott, R, additional, Wilson, S, additional, Leikis, R, additional, Nirmalaraj, BK, additional, Krzyżagórska, E, additional, Miękus, P, additional, Bronisz, M, additional, Mirek-Bryniarska, E, additional, Łanda, K, additional, Stasiewski, A, additional, Żechowicz, T, additional, Zytkiewicz-Jaruga, D, additional, Korecki, J, additional, Ogórek, M, additional, Pawłowicz, L, additional, Piepiorka, M, additional, Skierkowska, J, additional, Stankiewicz, A, additional, Szyprowska, E, additional, Witek, R, additional, Bochenek, A, additional, Kończakowski, P, additional, Wojnowski, Ł, additional, Wujkowski, M, additional, Cymerman, K, additional, Korzeniak, R, additional, Mąder, P, additional, Mikłaszewicz, B, additional, Stachlewski, P, additional, Goch, A, additional, Pomiećko, W, additional, Skórski, M, additional, Romanowski, L, additional, Jusiak, K, additional, Laskowska-Derlaga, E, additional, Bijata-Bronisz, R, additional, Kaźmierczak, J, additional, Goldberg, R, additional, Henderson, D, additional, Korban, E, additional, Rohr, K, additional, Claxton, E, additional, Weiss, R, additional, Angiolillo, D, additional, Boccalandro, F, additional, Chu, K, additional, Thorn, E, additional, Randhawa, P, additional, Singh, N, additional, Bittar, G, additional, Guarnieri, T, additional, Saeed, S, additional, Sharma, S, additional, Shepard, M, additional, French, W, additional, Desai, P, additional, Bernstein, R, additional, Rogers, W, additional, Singal, R, additional, Schneider, R, additional, Shanes, J, additional, Ong, S, additional, Condit, J, additional, Donahoe, S, additional, Brill, D, additional, Einhorn, D, additional, Ebrahimi, R, additional, Labroo, A, additional, Graf, R, additional, Scott, J, additional, Hoekstra, J, additional, Jetty, P, additional, Luckasen, G, additional, O'Donnell, P, additional, Gonte, W, additional, Pomposini, D, additional, Quadrel, M, additional, Koren, M, additional, Schlager, D, additional, Schramm, E, additional, Singal, D, additional, Lupovitch, S, additional, Soni, A, additional, Seigel, P, additional, Roberts, J, additional, Soufer, J, additional, Reza, S, additional, Quinlan, E, additional, Moretto, T, additional, First, B, additional, Khan, M, additional, Chilka, S, additional, Colfer, H, additional, Teklinski, A, additional, Wallace-Wilding, K, additional, Ellison, H, additional, Muse, D, additional, Aronoff, S, additional, Higgins, A, additional, Patel, S, additional, Elinoff, V, additional, Karim, A, additional, Awasty, V, additional, Chuang, R, additional, Roseman, H, additional, Dugano-Daphnis, P, additional, Albert, M, additional, Sheikh, K, additional, Bays, H, additional, Kaster, S, additional, Goldstein, M, additional, Rubino, D, additional, Calatayud, G, additional, Snyder, H, additional, Williams, T, additional, Hershon, K, additional, Hagan, M, additional, Isserman, S, additional, Kahn, B, additional, Anderson, J, additional, Gimness, MP, additional, Raisinghani, A, additional, Christina, M, additional, Raikhel, M, additional, Gillespie, E, additional, Portnay, E, additional, Heiman, M, additional, Qureshi, M, additional, Lee, J, additional, Blonder, R, additional, Cucher, F, additional, Miller, G, additional, Kotlaba, D, additional, Cornett, G, additional, Beavins, J, additional, Augenbraun, C, additional, Reinhardt, S, additional, Bartkowiak, A, additional, Salacata, A, additional, Blevins, T, additional, Benjamin, S, additional, Diener, J, additional, George, W, additional, Barker, B, additional, Richwine, R, additional, Baldari, D, additional, Alfieri, A, additional, Barreto, A, additional, Zhang, L, additional, Shah, R, additional, Hendrix, E, additional, Subramaniyam, V, additional, Hurley, S, additional, Lillestol, M, additional, O'Donoghue, M, additional, Shayani, S, additional, Ryan, E, additional, Call, R, additional, Zemel, L, additional, Chang, A, additional, Kivitz, A, additional, Freyne, B, additional, Bland, V, additional, Shore, K, additional, Mostel, E, additional, Uzoaga, E, additional, Andrawis, N, additional, Gabra, N, additional, Ghitis, A, additional, Sabatino, K, additional, Browder, D, additional, Varma, S, additional, Smith, S, additional, Fink, R, additional, Aycock, GR, additional, Doty, WD, additional, Alfonso, T, additional, Eshaghian, S, additional, Karlsberg, R, additional, Zarich, S, additional, Landau, C, additional, McKenzie, M, additional, Krause, R, additional, Davis, W, additional, Haddad, T, additional, Voyce, S, additional, Alford, C, additional, LeDoux, J, additional, O'Dea, D, additional, Park, J, additional, Aroda, V, additional, Getaneh, A, additional, Graham, B, additional, Bhagwat, R, additional, Korn, D, additional, Ruoff, G, additional, Wiseman, A, additional, Lieber, I, additional, Fialkow, J, additional, Gonzalez-Campoy, JM, additional, Bayron, C, additional, Bertolet, B, additional, Lash, J, additional, Gerrish, C, additional, Robertson, D, additional, Rosenfeld, J, additional, Seidner, M, additional, Agaiby, J, additional, Silverfield, J, additional, Sugimoto, D, additional, Lubin, B, additional, Alhaddad, M, additional, Lui, H, additional, Lakin, G, additional, Chokshi, S, additional, Donovan, D, additional, Felten, W, additional, Minton, S, additional, Kimmelstiel, C, additional, Kuvin, J, additional, Still, C, additional, Byars, W, additional, Talano, J, additional, Desai, V, additional, Bradley, AJ, additional, Baker, S, additional, Chane, M, additional, Mercado, A, additional, Baron, S, additional, Harris, B, additional, Mayer, N, additional, Concha, M, additional, Carr, K, additional, Chaykin, L, additional, Willis, J, additional, Clay, A, additional, Fenstad, E, additional, Furda, J, additional, Peterson, P, additional, Chang, M, additional, Aronne, L, additional, Jones, D, additional, Prashad, R, additional, Benson, M, additional, Stegemoller, R, additional, Longshaw, K, additional, Saleh, J, additional, Jennings, W, additional, Detweiler, R, additional, Viswanath, D, additional, Patel, R, additional, Lederman, S, additional, Weinstein, D, additional, Korabathina, R, additional, Singh, V, additional, Rosen, J, additional, Estevez, R, additional, Levin, P, additional, McNeill, R, additional, Kalen, V, additional, Reed, J, additional, Ashley, R, additional, Herman, L, additional, Tsai, Y, additional, Kayne, D, additional, White, A, additional, Hussain, I, additional, Tami, L, additional, Cohen, K, additional, Robinson, J, additional, Fuchs-Ertman, D, additional, Platt, G, additional, Belardo, L, additional, Reddy, R, additional, Rosendorff, C, additional, Saba, F, additional, Powell, S, additional, Anderson, K, additional, Abidi, M, additional, Rezkalla, S, additional, Paraschos, A, 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2018
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