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Jainendra K. Jain

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(Redirected fromJainendra Jain)
Indian-American physicist (born 1960)
This article is about the physicist. For the screenwriter, seeJainendra Jain (screenwriter).

Jainendra K. Jain
Born (1960-01-17)January 17, 1960 (age 66)
Alma mater
Known forComposite fermions
Jain sequences
Jain states
AwardsOliver E. Buckley Condensed Matter Prize(2002)
member,National Academy of Sciences(2021)
Foreign FellowIndian National Science Academy(2025)
Wolf Prize in Physics(2025)
Scientific career
FieldsCondensed matter theory
Doctoral advisorPhilip B. Allen,Steven Kivelson

Jainendra K. Jain, is anIndian-Americanphysicist and the Evan Pugh University Professor and the Eberly Chair inPhysics at thePennsylvania State University. He received theOliver E. Buckley Prize of theAmerican Physical Society in 2002, was elected to theNational Academy of Sciences in 2021, and was selected Foreign Fellow of theIndian National Science Academy in 2024.[1] He was the co-recipient of 2025Wolf Prize in Physics along withJames P. Eisenstein andMordehai Heiblum.[2] Jain is known for his theoretical work onquantum many body systems, most notably for postulating particles known as thecomposite fermions.

Biography

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Jain received his primary, middle and high school education in a government school in the rural village ofSambhar,Rajasthan,[3][4] located at the eastern margin of Thar desert in India. He received bachelor's degree atMaharaja College, Jaipur,[5] his master's degree in physics atIndian Institute of Technology Kanpur[5] and PhD at theStony Brook University,[5] where he worked with Profs. Philip B. Allen andSteven Kivelson. After post-doctoral positions at theUniversity of Maryland and theYale University he returned to theStony Brook University as a faculty member in 1989. In 1998, he moved to thePennsylvania State University[1] as the firstErwin W. Mueller Professor ofPhysics.

Jain is a quantum physicist in the field ofcondensed matter theory with interests in strongly interacting electronic systems in low dimensions. As the originator of the exotic particles calledcomposite fermions, he pioneered and developed the composite fermion theory of thefractional quantum Hall effect and unified the fractional and the integralquantum Hall effects. His writings include a monographComposite Fermions,[6] published in 2007 by theCambridge University Press. He co-edited withBertrand Halperin a bookFractional Quantum Hall Effects: New Developments,[7] published in 2020 byWorld Scientific.[3]

Because of injuries sustained in a childhood accident, Jain walks with the aid of a prosthesis.[3][4] After being awarded theWolf Prize in Physics, he recounted his journey as: “Looking back, it is hard to believe how incredibly fortunate I have been. Growing up in a poor village in India, traumatized by an accident that left me on crutches with a lifelong disability, I did not think I would ever walk again or attend college, let alone pursue my dream of becoming a physicist.”[8] He creditsJaipur Foot with enabling him to continue education.[3]

Research

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Jain predicted that when two-dimensional electrons are subjected to a large magnetic field, they dress themselves with an even number of quantized vortices to form emergent particles termedcomposite fermions.[9] Composite fermions are pictured as electrons dressed with magnetic flux quanta, and are predicted to experience a substantially reduced magnetic field. Thus, the strongly correlated 2D electrons in a high magnetic field become weakly interacting composite fermions at a reduced magnetic field. Composite fermions correctly predict the rich phenomenology of this system originating from a variety of strongly correlated states of electrons, including the fractional quantum Hall states, the Fermi-liquid like metallic states, superconductor-like paired states, and crystal states.[10][11][12][13][14]

Jain theorized that the integer quantum Hall effect of composite fermions carrying 2p flux quanta shows as the fractional quantum Hall effect of electrons at fractions n/(2pn±1), where n and p are integers. These fractions, along with their hole partners 1 - n/(2pn±1), termed the Jain sequences, account for nearly all known fractional quantum Hall states, called the Jain states. Experimental evidence has been reported for four species of composite fermions, those with 2, 4, 6, and 8 flux quanta attached.[15][16][17]

Jain also constructed ansatz wave functions[9] for the fractional quantum Hall states, which were shown by him and his collaborators to be extremely accurate.[18][19][20] They demonstrated that the excited composite fermions, also called "quasiparticles", exhibit fractional charge and anyon statistics.[21] They generalized the composite-fermion framework to include the spin (or valley) degree of freedom[22][23][24] and to bilayers,[25] and successfully predicted the phase diagram of composite-fermion crystals.[26][27] They further showed that the residual interactions among composite fermions can cause pairing of composite fermions at even-denominator fractions in higher Landau levels,[28] in wide quantum wells,[29] or with large Landau-level mixing.[30] They examined the fractional quantum Hall effect of composite fermions to explain fractions such as 4/11 and 5/13.[31]

Jain also is the originator the "parton" construction,[32] which generates candidate fractional quantum Hall states beyond the Jain sequences and includes some of the earliest proposed non-Abelian states.[33] Several parton states beyond the standard Jain states have been shown to be experimentally relevant.[34][35]

Honors

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References

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  1. ^abcdefghi"Jainendra K Jain — Penn State Department of Physics".www.phys.psu.edu. Retrieved24 February 2018.
  2. ^Wolf Prize in Physics 2025
  3. ^abcdAhmed, Farooq (2022)."Profile of Jainendra K. Jain".Proceedings of the National Academy of Sciences.119 (30) e2208671119.Bibcode:2022PNAS..11908671A.doi:10.1073/pnas.2208671119.PMC 9335342.PMID 35858393.
  4. ^ab"'For us physicists, beauty is a new idea that unifies and explains'".Hindustan Times. 2 May 2025. Retrieved19 December 2025.
  5. ^abc"Array of contemporary American Physicists". American Institute of Physics. Retrieved20 October 2010.[permanent dead link]
  6. ^"Composite fermions".Cambridge University Press. Retrieved24 February 2018.
  7. ^Halperin, Bertrand I.; Jain, Jainendra K. (2020).Fractional Quantum Hall Effects: New Developments.arXiv:2011.13488.doi:10.1142/11751.ISBN 978-981-12-1748-7.
  8. ^"Jainendra Jain named 2025 Wolf Prize laureate in physics".
  9. ^abJ. K. Jain (1989)."Composite-fermion approach for the fractional quantum Hall effect".Physical Review Letters.doi:10.1103/PhysRevLett.63.199.
  10. ^Olle Heinonen (1998)."Composite fermions: a unified view of the quantum Hall regime".World Scientific.
  11. ^H. L. Stormer; D. C. Tsui (2007)."Composite fermions in the fractional quantum Hall effect".Perspectives in Quantum Hall Effects.doi:10.1002/9783527617258.ch10.{{cite web}}: CS1 maint: multiple names: authors list (link)
  12. ^J. K. Jain (2020)."Thirty Years of Composite Fermions and Beyond".Fractional Quantum Hall Effects: New Developments.doi:10.1142/9789811217494_0001.
  13. ^B.I. Halperin (2020)."The Half-Full Landau Level".Fractional Quantum Hall Effects: New Developments.doi:10.1142/9789811217494_0001.
  14. ^M. Shayegan (2020)."Probing Composite Fermions Near Half-Filled Landau Level".Fractional Quantum Hall Effects: New Developments.doi:10.1142/9789811217494_0001.
  15. ^W. Pan, H.L. Stormer, D. C. Tsui, L.N. Pfeiffer, K.W. Baldwin, K.W. West (2002)."Transition from an electron solid to the sequence of fractional quantum Hall states at very low Landau level filling factor".Phys. Rev. Lett.doi:10.1103/PhysRevLett.88.176802.{{cite web}}: CS1 maint: multiple names: authors list (link)
  16. ^Y. Huang, W. Hussain, S.A. Myers, L.N. Pfeiffer, K.W. West, K.W. Baldwin, G.A. Csathy (2024)."Evidence for Topological Protection Derived from Six-Flux Composite Fermions".{{cite web}}: CS1 maint: multiple names: authors list (link)
  17. ^Y. J. Chung, D. Graf, L.W. Engel, K.A. Villegas Rosales, P.T. Madathil, K.W. Baldwin, K. W. West, L. N. Pfeiffer, and M. Shanegan (2022)."Correlated states of 2D electrons near ν = 1/7".doi:10.1103/PhysRevLett.128.026802.{{cite web}}: CS1 maint: multiple names: authors list (link)
  18. ^Jain, Jainendra K. (1997)."Composite fermions in the Hilbert space of the lowest electronic Landau level".doi:10.1142/S0217979297001301.
  19. ^Gautam Dev; J. K. Jain (1992)."Band structure of the fractional quantum Hall effect".doi:10.1103/PhysRevLett.69.2843.{{cite web}}: CS1 maint: multiple names: authors list (link)
  20. ^A. C. Balram; A. Wójs; J. K. Jain (2013)."State counting for excited bands of the fractional quantum Hall effect".doi:10.1103/PhysRevB.88.205312.{{cite web}}: CS1 maint: multiple names: authors list (link)
  21. ^G. S. Jeon; K. L. Graham; J. K. Jain (2004)."Berry phases for composite fermions".doi:10.1103/PhysRevB.70.125316.{{cite web}}: CS1 maint: multiple names: authors list (link)
  22. ^X. G. Wu; G. Dev; J. K. Jain (1993)."Mixed-spin incompressible states in the fractional quantum Hall effect".doi:10.1103/PhysRevLett.71.153.{{cite web}}: CS1 maint: multiple names: authors list (link)
  23. ^K. Park; J. K. Jain (1998)."Phase diagram of the spin polarization of composite fermions".doi:10.1103/PhysRevLett.80.4237.{{cite web}}: CS1 maint: multiple names: authors list (link)
  24. ^Y. Zhang; A. Wójs; J. K. Jain (2016)."Landau-level mixing and particle-hole symmetry breaking".doi:10.1103/PhysRevLett.117.116803.{{cite web}}: CS1 maint: multiple names: authors list (link)
  25. ^V. W. Scarola; J. K. Jain (2001)."Phase diagram of bilayer composite fermion states".doi:10.1103/PhysRevB.64.085313.{{cite web}}: CS1 maint: multiple names: authors list (link)
  26. ^A. C. Archer; K. Park; J. K. Jain (2013)."Competing crystal phases in the lowest Landau level".doi:10.1103/PhysRevLett.111.146804.{{cite web}}: CS1 maint: multiple names: authors list (link)
  27. ^J. Zhao; Y. Zhang; J. K. Jain (2018)."Crystallization in the fractional quantum Hall regime induced by Landau-level mixing".doi:10.1103/PhysRevLett.121.116802.{{cite web}}: CS1 maint: multiple names: authors list (link)
  28. ^A. Sharma; S. Pu; A. C. Balram; J. K. Jain (2023)."Fractional quantum Hall effect with unconventional pairing in monolayer graphene".doi:10.1103/PhysRevLett.130.126201.{{cite web}}: CS1 maint: multiple names: authors list (link)
  29. ^A. Sharma; A. C. Balram; J. K. Jain (2024)."Composite-fermion pairing at half- and quarter-filled lowest Landau level".doi:10.1103/PhysRevB.109.035306.{{cite web}}: CS1 maint: multiple names: authors list (link)
  30. ^T. Zhao; A. C. Balram; J. K. Jain (2023)."Composite fermion pairing induced by Landau-level mixing".doi:10.1103/PhysRevLett.130.186302.{{cite web}}: CS1 maint: multiple names: authors list (link)
  31. ^S. Mukherjee, S.S. Mandal, Y.H. Wu, A. Wojs, J.K. Jain (2014)."Enigmatic 4/11 state: A prototype for unconventional fractional quantum Hall effect".doi:10.1103/PhysRevLett.112.016801.{{cite web}}: CS1 maint: multiple names: authors list (link)
  32. ^J. K. Jain (1989)."Incompressible quantum Hall states".doi:10.1103/PhysRevB.40.8079.
  33. ^X.-G. Wen (1991)."Non-abelian statistics in the fractional quantum Hall states".doi:10.1103/PhysRevLett.66.802.
  34. ^A. C. Balram; M. Barkeshli; M. S. Rudner (2018)."Parton construction of a wave function in the anti-Pfaffian phase".doi:10.1103/PhysRevB.98.035127.{{cite web}}: CS1 maint: multiple names: authors list (link)
  35. ^A. C. Balram, S. Mukherjee, K. Park, M. Barkeshli, M.S. Rudner, J.K. Jain (2018)."Fractional quantum Hall effect at ν = 2 + 6/13: The parton paradigm for the second Landau level".doi:10.1103/PhysRevLett.121.186601.{{cite web}}: CS1 maint: multiple names: authors list (link)
  36. ^"Buckley Prize".www.aps.org. Retrieved24 February 2018.
  37. ^"AAAS Fellow".
  38. ^"Evan Pugh University Professors".
  39. ^"2021 NAS Election".
  40. ^"INSA Foreign Fellows elected".
  41. ^Wolf Prize in Physics 2025
Laureates of theWolf Prize in Physics
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