@article {238, title = {Linear dichroism infrared resonance in overdoped, underdoped, and optimally doped cuprate superconductors}, journal = {Physical Review B}, volume = {102}, number = {5}, year = {2020}, note = {ISI Document Delivery No.: NE5GO
Times Cited: 0
Cited Reference Count: 30
Cited References:
Acbas G, 2009, PHYS REV LETT, V103, DOI 10.1103/PhysRevLett.103.137201
Armitage NP, 2014, PHYS REV B, V90, DOI 10.1103/PhysRevB.90.035135
Arpaia R, 2018, PHY REV MATER, V2, DOI 10.1103/PhysRevMaterials.2.024804
Basov DN, 2005, REV MOD PHYS, V77, P721, DOI 10.1103/RevModPhys.77.721
Blumberg G, 1996, PHYS REV B, V53, P11930, DOI 10.1103/PhysRevB.53.R11930
Cerne J, 2000, PHYS REV LETT, V84, P3418, DOI 10.1103/PhysRevLett.84.3418
Fauque B, 2006, PHYS REV LETT, V96, DOI 10.1103/PhysRevLett.96.197001
Fridman I, 2011, PHYS REV B, V84, DOI 10.1103/PhysRevB.84.104522
George DK, 2012, J OPT SOC AM B, V29, P1406, DOI 10.1364/JOSAB.29.001406
Halperin B. I., 1991, SPRINGER P PHYS, V60, P439
Humlicek J, 2000, PHYS REV B, V61, P14554, DOI 10.1103/PhysRevB.61.14554
KOREN G, 1989, APPL PHYS LETT, V54, P1054, DOI 10.1063/1.101559
Koren G, 2016, PHYS REV B, V94, DOI 10.1103/PhysRevB.94.174515
Lubashevsky Y, 2014, PHYS REV LETT, V112, DOI 10.1103/PhysRevLett.112.147001
Mukherjee A, 2019, PHYS REV B, V99, DOI 10.1103/PhysRevB.99.085440
Nie LM, 2014, P NATL ACAD SCI USA, V111, P7980, DOI 10.1073/pnas.1406019111
Orenstein J, 2011, PHYS REV LETT, V107, DOI 10.1103/PhysRevLett.107.067002
PISAREV RV, 1991, PHASE TRANSIT, V37, P63, DOI 10.1080/01411599108203448
Simon ME, 2002, PHYS REV LETT, V89, DOI 10.1103/PhysRevLett.89.247003
TROFIMOV IE, 1994, APPL PHYS LETT, V65, P2481, DOI 10.1063/1.112671
Varma CM, 2014, EPL-EUROPHYS LETT, V106, DOI 10.1209/0295-5075/106/27001
Varma CM, 1997, PHYS REV B, V55, P14554, DOI 10.1103/PhysRevB.55.14554
Wu J, 2017, NATURE, V547, P432, DOI 10.1038/nature23290
Xia J, 2008, PHYS REV LETT, V100, DOI 10.1103/PhysRevLett.100.127002
Yakes MK, 2010, NANO LETT, V10, P1559, DOI 10.1021/nl9035302
Yakovenko VM, 2015, PHYSICA B, V460, P159, DOI 10.1016/j.physb.2014.11.060
Zhang H, 2018, PHYS REV MATER, V2, DOI 10.1103/PhysRevMaterials.2.033803
Zhang J, 2018, SCI ADV, V4, DOI 10.1126/sciadv.aao5235
Zhao L, 2017, NAT PHYS, V13, P250, DOI [10.1038/nphys3962, 10.1038/NPHYS3962]
Zhao L., 2018, ENCY MODERN OPTICS, P207
Mukherjee, A. Seo, J. Arik, M. M. Zhang, H. Zhang, C. C. Kirzhner, T. George, D. K. Markelz, A. G. Armitage, N. P. Koren, G. Wei, J. Y. T. Cerne, J.
NSF-DMR GrantNational Science Foundation (NSF) [1410599]; NSFNational Science Foundation (NSF) [MCB 1616529, DMR 1905519]; DOEUnited States Department of Energy (DOE) [DE-SC0016317]; NSERCNatural Sciences and Engineering Research Council of Canada (NSERC); CFI-OITCanada Foundation for Innovation; Canadian Institute for Advanced ResearchCanadian Institute for Advanced Research (CIFAR)
We are indebted to D. Hsieh, S. A. Kivelson, C. M. Varma, and L. Zhao for helpful discussions. We gratefully acknowledge support from NSF-DMR Grant No. 1410599 (J.C.). A.G.M. and D.K.G. were supported by NSF Grant No. MCB 1616529 and DOE Grant No. DE-SC0016317. Work in Toronto was supported by NSERC, CFI-OIT, and the Canadian Institute for Advanced Research. J.Y.T.W. thanks Kejun Xu for laboratory assistance in Toronto. N.P.A. was supported by NSF Grant No. DMR 1905519.

9
Amer physical soc
College pk
2469-9969}, month = {Aug}, pages = {6}, type = {Article}, abstract = {

By measuring the polarization changes in terahertz, infrared, and visible radiation over an extended energy range (3-2330 meV), we observe symmetry breaking in cuprate high-temperature superconductors over wide energy, doping, and temperature ranges. We measure the polarization rotation (Re[theta(F)]) and ellipticity (Im[theta(F)]) of transmitted radiation through thin films as the sample is rotated. We observe a twofold rotational symmetry in theta(F), which is associated with linear dichroism (LD) and occurs when electromagnetic radiation polarized along one direction is absorbed more strongly than radiation polarized in the perpendicular direction. Such polarization anisotropies can be generally associated with symmetry breakings. We measure the amplitude of the LD signal and study its temperature, energy, and doping dependence. The LD signal shows a resonant behavior with a peak in the few hundred meV range, which is coincident with the midinfrared optical feature that has been associated with the formation of the pseudogap state. The strongest LD signal is found in underdoped films, although it is also observed in optimally and overdoped samples. The LD signal is consistent with an electronic nematic order which is decoupled from the crystallographic axes as well as novel magnetoelectric effects.

}, keywords = {Materials Science, Physics}, isbn = {2469-9950}, doi = {10.1103/PhysRevB.102.054520}, author = {Mukherjee, A. and Seo, J. and Arik, M. M. and Zhang, H. and Zhang, C. C. and Kirzhner, T. and George, D. K. and Markelz, A. G. and Armitage, N. P. and Koren, G. and Wei, J. Y. T. and Cerne, J.} } @proceedings {307, title = {Multi-component response in multilayer graphene revealed through terahertz and infrared magneto-spectroscopy}, year = {2012}, month = {9/2012}, address = {Wollongong, Australia}, doi = {10.1109/IRMMW-THz.2012.6380102}, author = {Ellis, C. T. and Stier, A. V. and George, D. K. and Tischler, J. G. and Glaser, E. R. and Myers-Ward, R. L. and Tedesco, J. L. and Eddy, C. R. and Gaskill, D. K. and Markelz, A. G. and Cerne, J.} } @article {221, title = {Terahertz Response and Colossal Kerr Rotation from the Surface States of the Topological Insulator Bi2Se3}, journal = {Physical Review Letters}, volume = {108}, number = {8}, year = {2012}, note = {ISI Document Delivery No.: 896NY
Times Cited: 164
Cited Reference Count: 35
Cited References:
Akhmerov AR, 2009, PHYS REV LETT, V102, DOI 10.1103/PhysRevLett.102.216404
Alpichshev Z, 2010, PHYS REV LETT, V104, DOI 10.1103/PhysRevLett.104.016401
Analytis JG, 2010, PHYS REV B, V81, DOI 10.1103/PhysRevB.81.205407
Bansal N., ARXIV11045709
Benia HM, 2011, PHYS REV LETT, V107, DOI 10.1103/PhysRevLett.107.177602
Bianchi M, 2010, NAT COMMUN, V1, DOI 10.1038/ncomms1131
Butch NP, 2010, PHYS REV B, V81, DOI 10.1103/PhysRevB.81.241301
Chen J, 2011, PHYS REV B, V83, DOI 10.1103/PhysRevB.83.241304
Chen YL, 2009, SCIENCE, V325, P178, DOI 10.1126/science.1173034
Essin AM, 2009, PHYS REV LETT, V102, DOI 10.1103/PhysRevLett.102.146805
Eto K, 2010, PHYS REV B, V81, DOI 10.1103/PhysRevB.81.195309
Fu L, 2007, PHYS REV B, V76, DOI 10.1103/PhysRevB.76.045302
Fu L, 2008, PHYS REV LETT, V100, DOI 10.1103/PhysRevLett.100.096407
Hsieh D, 2008, NATURE, V452, P970, DOI 10.1038/nature06843
Hsieh D, 2009, NATURE, V460, P1101, DOI 10.1038/nature08234
Jenkins GS, 2010, PHYS REV B, V82, DOI 10.1103/PhysRevB.82.125120
King PDC, 2011, PHYS REV LETT, V107, DOI 10.1103/PhysRevLett.107.096802
LaForge AD, 2010, PHYS REV B, V81, DOI 10.1103/PhysRevB.81.125120
Lan YP, 2011, PHYS REV B, V83, DOI 10.1103/PhysRevB.83.205109
Maciejko J, 2010, PHYS REV LETT, V105, DOI 10.1103/PhysRevLett.105.166803
Moore JE, 2007, PHYS REV B, V75, DOI 10.1103/PhysRevB.75.121306
Qi XL, 2008, PHYS REV B, V78, DOI 10.1103/PhysRevB.78.195424
Qu DX, 2010, SCIENCE, V329, P821, DOI 10.1126/science.1189792
Roushan P, 2009, NATURE, V460, P1106, DOI 10.1038/nature08308
Roy R, 2009, PHYS REV B, V79, DOI 10.1103/PhysRevB.79.195322
Steinberg H, 2011, PHYS REV B, V84, DOI 10.1103/PhysRevB.84.233101
Sushkov AB, 2010, PHYS REV B, V82, DOI 10.1103/PhysRevB.82.125110
THOULESS DJ, 1982, PHYS REV LETT, V49, P405, DOI 10.1103/PhysRevLett.49.405
Tkachov G, 2011, PHYS REV B, V84, DOI 10.1103/PhysRevB.84.035405
Tse WK, 2010, PHYS REV B, V82, DOI 10.1103/PhysRevB.82.161104
Tse WK, 2010, PHYS REV LETT, V105, DOI 10.1103/PhysRevLett.105.057401
VONKLITZING K, 1980, PHYS REV LETT, V45, P494, DOI 10.1103/physrevlett.45.494
Xia Y, 2009, NAT PHYS, V5, P398, DOI 10.1038/NPHYS1274
Xiong J., PHYSICA A E IN PRESS
Zhang XA, 2010, PHYS REV B, V82, DOI 10.1103/PhysRevB.82.245107
Aguilar, R. Valdes Stier, A. V. Liu, W. Bilbro, L. S. George, D. K. Bansal, N. Wu, L. Cerne, J. Markelz, A. G. Oh, S. Armitage, N. P.
George, Deepu/J-9882-2014; Aguilar, Rolando Valdes/A-6637-2012; Liu, Wei/H-5999-2012; Wu, Liang/C-8715-2015
George, Deepu/0000-0003-0021-0705; Aguilar, Rolando Valdes/0000-0002-4321-4792; Wu, Liang/0000-0003-1696-7809; Markelz, Andrea/0000-0003-0443-4319
"Institute for Quantum Matter" DOE [DE-FG02-08ER46544]; Gordon and Betty Moore FoundationGordon and Betty Moore Foundation; NSFNational Science Foundation (NSF) [MRI-R2 0959989, DMR-1006078, DMR-0845464]; IAMDN of Rutgers University; ONROffice of Naval Research [N000140910749]; Division Of Materials ResearchNational Science Foundation (NSF)NSF - Directorate for Mathematical \& Physical Sciences (MPS) [0845464] Funding Source: National Science Foundation
The authors would like to thank H. D. Drew, J. Hancock, Z. Hao, G. S. Jenkins, A. Kuzmenko, A. MacDonald, N. A. Mecholsky, A. J. Pearson, O. Tchernyshyov, W-K. Tse, and Y. Wan for helpful discussions and/or correspondences. Support for the measurements at JHU was provided under the auspices of the "Institute for Quantum Matter" DOE DE-FG02-08ER46544 and the Gordon and Betty Moore Foundation. The work at UB was supported by NSF MRI-R2 0959989 and NSF DMR-1006078. The work at Rutgers was supported by IAMDN of Rutgers University, NSF DMR-0845464 and ONR N000140910749.
166
3
157
Amer physical soc
College pk}, month = {Feb}, pages = {5}, type = {Article}, abstract = {

We report the THz response of thin films of the topological insulator Bi2Se3. At low frequencies, transport is essentially thickness independent showing the dominant contribution of the surface electrons. Despite their extended exposure to ambient conditions, these surfaces exhibit robust properties including narrow, almost thickness-independent Drude peaks, and an unprecedentedly large polarization rotation of linearly polarized light reflected in an applied magnetic field. This Kerr rotation can be as large as 65 degrees and can be explained by a cyclotron resonance effect of the surface states.

}, keywords = {bi2te3, Physics}, isbn = {0031-9007}, doi = {https://doi.org/10.1103/physrevlett.108.087403}, author = {Aguilar, R. V. and Stier, A. V. and Liu, W. and Bilbro, L. S. and George, D. K. and Bansal, N. and Wu, L. and Cerne, J. and Markelz, A. G. and Oh, S. and Armitage, N. P.} } @proceedings {244, title = {Magneto Optical Polarization Measurements using THz Polarization Modulation Spectroscopy}, year = {2011}, note = {ISI Document Delivery No.: BJT73
Times Cited: 0
Cited Reference Count: 3
Cited References:
Cerne J, 2000, PHYS REV B, V61, P8133, DOI 10.1103/PhysRevB.61.8133
Crassee I, 2011, NAT PHYS, V7, P48, DOI 10.1038/NPHYS1816
Tse WK, 2010, PHYS REV LETT, V105, DOI 10.1103/PhysRevLett.105.057401
Stier, A. V. George, D. Markelz, A. G. Cerne, J.
Irmmw-thz
Proceedings Paper
36th International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW-THz)
Oct 02-07, 2011
Houston, TX
Rice Univ, IEEE Microwave Theory \& Tech Soc, NASA, California Inst Technol, Jet Prop Lab, Univ Wollongong
George, Deepu/J-9882-2014
George, Deepu/0000-0003-0021-0705
345 e 47th st, new york, ny 10017 usa
2162-2027}, publisher = {Ieee}, address = {New York}, abstract = {

We report a new broad band technique for rapidly measuring the complex Faraday and Kerr rotations in materials such as topological insulators and graphene, combining the distinct advantages of THz time domain spectroscopy and polarization modulation techniques. The performance of the system is demonstrated using GaAs two dimensional electron gas in a magnetic field.

}, isbn = {978-1-4577-0509-0}, doi = {10.1364/JOSAB.29.001406}, author = {Stier, A. V. and George, D. and Markelz, A. G. and Cerne, J.}, editor = {Koch, M.} } @article {263, title = {Large oxidation dependence observed in terahertz dielectric response for cytochrome c}, journal = {Physical Review E}, volume = {72}, number = {4}, year = {2005}, note = {ISI Document Delivery No.: 979GO
Times Cited: 51
Cited Reference Count: 29
Cited References:
BERGHUIS AM, 1992, J MOL BIOL, V223, P959, DOI 10.1016/0022-2836(92)90255-I
BONE S, 1985, J MOL BIOL, V181, P323, DOI 10.1016/0022-2836(85)90096-8
BONE S, 1982, J MOL BIOL, V157, P571, DOI 10.1016/0022-2836(82)90477-6
BROOKS B, 1985, P NATL ACAD SCI USA, V82, P4995, DOI 10.1073/pnas.82.15.4995
Brucherseifer M, 2000, APPL PHYS LETT, V77, P4049, DOI 10.1063/1.1332415
Carlson HA, 2002, CURR OPIN CHEM BIOL, V6, P447, DOI 10.1016/S1367-5931(02)00341-1
CHEN JY, IN PRESS BIOPHYS J
CUSACK S, 1986, PHYSICA B \& C, V136, P256, DOI 10.1016/S0378-4363(86)80069-9
EDEN D, 1982, P NATL ACAD SCI-BIOL, V79, P815, DOI 10.1073/pnas.79.3.815
FROHWIRT EM, 1959, BIOPHYS J, V71, P570
Jackson J.D., 1975, CLASSICAL ELECTRODYN
KOPPENOL WH, 1982, J BIOL CHEM, V257, P4426
Kutteruf MR, 2003, CHEM PHYS LETT, V375, P337, DOI 10.1016/S0009-2614(03)00856-X
Markelz A, 2002, PHYS MED BIOL, V47, P3797, DOI 10.1088/0031-9155/47/21/318
Markelz AG, 2000, CHEM PHYS LETT, V320, P42, DOI 10.1016/S0009-2614(00)00227-X
Menikh A, 2004, BIOSENS BIOELECTRON, V20, P658, DOI 10.1016/j.bios.2004.03.006
Nagel M, 2002, APPL PHYS LETT, V80, P154, DOI 10.1063/1.1428619
PETHIG R, 1979, DIELECTRIC ELECTRONI
Qi PXR, 1996, BIOCHEMISTRY-US, V35, P12275, DOI 10.1021/bi961042w
RINGE D, 1985, PROG BIOPHYS MOL BIO, V45, P197, DOI 10.1016/0079-6107(85)90002-1
SHECHTER E, 1967, BIOPOLYMERS, V5, P788, DOI 10.1002/bip.1967.360050812
SIMONSON T, 1995, P NATL ACAD SCI USA, V92, P1082, DOI 10.1073/pnas.92.4.1082
SREENATHAN BR, 1971, BIOCHEM BIOPH RES CO, V42, P1122, DOI 10.1016/0006-291X(71)90021-0
Takano T., 1984, Methods and Applications in Crystallographic Computing. International Summer School on Crystallographic Computing, P262
TAKANO T, 1980, P NATL ACAD SCI-BIOL, V77, P6371, DOI 10.1073/pnas.77.11.6371
Whitmire SE, 2003, BIOPHYS J, V85, P1269, DOI 10.1016/S0006-3495(03)74562-7
WHITMIRE SE, 2003, SENSING SCI ELECT TE, V2
Yamamoto K, 2002, B CHEM SOC JPN, V75, P1083, DOI 10.1246/bcsj.75.1083
Zhang CF, 2004, J PHYS CHEM B, V108, P10077, DOI 10.1021/jp049933y
Chen, JY Knab, JR Cerne, J Markelz, AG
Markelz, Andrea/0000-0003-0443-4319
52

22
Amer physical soc
College pk
1550-2376
1}, month = {Oct}, pages = {4}, type = {Article}, abstract = {

Far infrared dielectric response is used to characterize the collective mode density of states for cytochrome c as a function of oxidation state and hydration using terahertz time domain spectroscopy. A strong absorbance and refractive index increase was observed with the oxidation. A simple phenomenological fitting using a continuous distribution of oscillators reproduces the frequency dependence of the complex dielectric response as well as demonstrates quantitative agreement with a uniform increase in either mode density or polarizability with oxidation in the 5-80 cm(-1) frequency range. Hydration dependence measurements find that a difference in the equilibrium water content for ferri and ferro cytochrome c is not sufficient to account for the large change in terahertz response. The large dielectric increase at terahertz frequencies with oxidation suggests either a significant global softening of the potential and/or a significant increase in polarizability with oxidation.

}, keywords = {absorption, binding, conformation, dna, dynamics, heart ferricytochrome-c, modes, Physics, protein flexibility, spectroscopy, state}, isbn = {1539-3755}, doi = {10.1103/PhysRevE.72.040901}, author = {Chen, J. Y. and Knab, J. R. and Cerne, J. and Markelz, A. G.} } @proceedings {310, title = {Terahertz measurements of the Photoactive Protein Bacteriorhodopsin mutant D96N: M and P states}, volume = {826}, year = {2004}, pages = {pages261{\textendash}267}, address = {Warrendale, PA}, abstract = {

We use terahertz (THz) spectroscopy as a biomaterials characterization tool. Previously we have shown a strong contrast between the THz dielectric response for wild type (WT) and D96N mutant of bacteriorhodopsin. In those studies we observed a large increase in the THz absorbance of WT with excitation to thermally captured photo-intermediates whereas no such increase in absorbance was observed for the mutant D96N. These results suggest that the THz response is sensitive to structural changes and relative flexibility of biomolecules. However the photo-intermediate populations of the WT and D96N samples were not equivalent in those measurements. While the WT samples had relaxed (bR), M and P state intermediates present, the D96N samples had only bR and M states. Here we present terahertz absorbance measurements of D96N as a function of M and P state populations at room temperature. The THz response is constant for intermediate states populations up to 23\% M state and up to 30\% P state. These results verify that there is a fundamental difference in the conformational dynamics as measured by THz dielectric response for a single residue mutation.

}, doi = {10.1557/PROC-826-V2.6}, author = {Chen, C.-Y. and Knab, J. R. and Cerne, J. and Hillebrecht, J. R. and Birge, R. R. and Markelz, A. G.} } @proceedings {313, title = {Biosensing with Terahertz Spectroscopy: Ligand Binding Effects}, year = {2003}, address = {Santa Barbara, CA}, author = {Chen, J.-Y. and Cerne, J. and Markelz, A. G.} } @proceedings {314, title = {Terahertz Biosensors based on Xerogel Substrates}, year = {2003}, address = {Santa Barbara, CA}, author = {Chen, J.-Y. and Cox, W. and Bright, F. V. and Cerne, J. and Markelz, A. G.} } @article {258, title = {Temperature of quasi-two-dimensional electron gases under steady-state terahertz drive}, journal = {Applied Physics Letters}, volume = {68}, number = {6}, year = {1996}, note = {ISI Document Delivery No.: TT663
Times Cited: 59
Cited Reference Count: 12
Cited References:
ASMAR NG, 1995, PHYS REV B, V51, P18041, DOI 10.1103/PhysRevB.51.18041
BETHUNE DS, 1989, J OPT SOC AM B, V6, P910, DOI 10.1364/JOSAB.6.000910
CERNE J, 1995, PHYS REV B, V51, P5253, DOI 10.1103/PhysRevB.51.5253
CONWELL E, 1967, SOLID STATE PHYS S, V9
GUPTA R, 1992, PHYS REV B, V46, P7745, DOI 10.1103/PhysRevB.46.7745
HEYMAN JN, 1994, PHYS REV LETT, V72, P2183, DOI 10.1103/PhysRevLett.72.2183
KOMIYAMA S, 1985, PHYS REV B, V32, P5532, DOI 10.1103/PhysRevB.32.5532
MARKELZ AG, 1994, SOLID STATE ELECTRON, V37, P1243, DOI 10.1016/0038-1101(94)90399-9
MARKELZ AG, 1995, THESIS U CALIFORNIA
SHAH J, 1984, APPL PHYS LETT, V44, P322, DOI 10.1063/1.94739
SHAH J, 1978, SOLID STATE ELECTRON, V21, P43, DOI 10.1016/0038-1101(78)90113-2
YANG CH, 1985, PHYS REV LETT, V55, P2359, DOI 10.1103/PhysRevLett.55.2359
Asmar, NG Cerne, J Markelz, AG Gwinn, EG Sherwin, MS Campman, KL Gossard, AC
Sherwin, Mark S/Q-4762-2017
Sherwin, Mark S/0000-0002-3869-1893; Markelz, Andrea/0000-0003-0443-4319
59

7
Amer inst physics
Woodbury}, month = {Feb}, pages = {829-831}, type = {Article}, abstract = {

We use photoluminescence to study the time-average energy distribution of electrons in the presence of strong steady-state drive at terahertz (THz) frequencies, in a modulation-doped 125 Angstrom AlGaAs/GaAs square well that is held at low lattice temperature TL. We find that the energy distribution can be characterized by an effective electron temperature, T-e(\>T-L), that agrees well with values estimated from the THz-illuminated, dc conductivity. This agreement indicates that under strong THz drive, LO phonon scattering dominates both energy and momentum relaxation; that the carrier distribution maintains a heated, thermal form; and that phonon drift effects are negligible. (C) 1996 American Institute of Physics.

}, keywords = {hot-electrons, Physics}, isbn = {0003-6951}, doi = {10.1063/1.116547}, author = {Asmar, N. G. and Cerne, J. and Markelz, A. G. and Gwinn, E. G. and Sherwin, M. S. and Campman, K. L. and Gossard, A. C.} } @article {262, title = {QUENCHING OF EXCITONIC QUANTUM-WELL PHOTOLUMINESCENCE BY INTENSE FAR-INFRARED RADIATION - FREE-CARRIER HEATING}, journal = {Physical Review B}, volume = {51}, number = {8}, year = {1995}, note = {Sherwin, Mark S/Q-4762-2017
Sherwin, Mark S/0000-0002-3869-1893; Markelz, Andrea/0000-0003-0443-4319
29}, month = {Feb 15}, pages = {5253-5262}, isbn = {0163-1829}, doi = {10.1103/PhysRevB.51.5253}, author = {Cerne, J. and Markelz, A. G. and Sherwin, M. S. and Allen, S. J. and Sundaram, M. and Gossard, A. C. and Vanson, P. C. and Bimberg, D.} } @article {259, title = {RESONANT-ENERGY RELAXATION OF TERAHERTZ-DRIVEN 2-DIMENSIONAL ELECTRON GASES}, journal = {Physical Review B}, volume = {51}, number = {24}, year = {1995}, note = {Sherwin, Mark S/Q-4762-2017
Sherwin, Mark S/0000-0002-3869-1893; Markelz, Andrea/0000-0003-0443-4319
119}, month = {Jun 15}, pages = {18041-18044}, isbn = {0163-1829}, doi = {10.1103/PhysRevB.51.18041}, author = {Asmar, N. G. and Markelz, A. G. and Gwinn, E. G. and Cerne, J. and Sherwin, M. S. and Campman, K. L. and Hopkins, P. F. and Gossard, A. C.} } @proceedings {318, title = {Frequency Dependence of the Third Order Susceptibility of InAs Quantum Wells at Terahertz Frequencies}, year = {1994}, month = {08/1994}, pages = {1193-1196}, author = {Markelz, A.G. and Cerne, J. and Gwinn, E. G. and Brar, B. and Kroemer, H.} }