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Gerard 't Hooft

Gerardus (Gerard) 't Hooft (Dutch: [ˈɣeːrɑrt ət ˈɦoːft]; born July 5, 1946) is a Dutch theoretical physicist and professor at Utrecht University, the Netherlands. He shared the 1999 Nobel Prize in Physics with his thesis advisor Martinus J. G. Veltman "for elucidating the quantum structure of electroweak interactions".

Gerard 't Hooft
't Hooft in November 2008
Born (1946-07-05) July 5, 1946 (age 76)
Den Helder, Netherlands
NationalityDutch
Alma materUtrecht University
Known forQuantum field theory
Quantum gravity
't Hooft condition
't Hooft–Polyakov monopole
't Hooft symbol
't Hooft loop
Feynman–'t Hooft gauge
Black hole complementarity
Minimal subtraction scheme
Holographic principle
Renormalization of Yang–Mills theory
Dimensional regularization
Renormalon
1/N expansion
AwardsHeineman Prize (1979)
Wolf Prize (1981)
Lorentz Medal (1986)
Spinoza Prize (1995)
Franklin Medal (1995)
Nobel Prize in Physics (1999)
High Energy and Particle Physics Prize (1999)
Lomonosov Gold Medal (2010)
Scientific career
FieldsTheoretical physics
InstitutionsUtrecht University
Doctoral advisorMartinus J. G. Veltman
Doctoral studentsRobbert Dijkgraaf
Herman Verlinde
Max Welling

His work concentrates on gauge theory, black holes, quantum gravity and fundamental aspects of quantum mechanics. His contributions to physics include a proof that gauge theories are renormalizable, dimensional regularization and the holographic principle.

Personal life

He is married to Albertha Schik (Betteke) and has two daughters.

Biography

Early life

Gerard 't Hooft was born in Den Helder on July 5, 1946,[1] but grew up in The Hague. He was the middle child of a family of three. He comes from a family of scholars. His great uncle was Nobel prize laureate Frits Zernike, and his grandmother was married to Pieter Nicolaas van Kampen, a professor of zoology at Leiden University. His uncle Nico van Kampen was an (emeritus) professor of theoretical physics at Utrecht University, and his mother married a maritime engineer.[2] Following his family's footsteps, he showed interest in science at an early age. When his primary school teacher asked him what he wanted to be when he grew up, he replied, "a man who knows everything."[2]

After primary school Gerard attended the Dalton Lyceum, a school that applied the ideas of the Dalton Plan, an educational method that suited him well. He excelled at science and mathematics courses. At the age of sixteen he won a silver medal in the second Dutch Math Olympiad. [2]

Education

After Gerard 't Hooft passed his high school exams in 1964, he enrolled in the physics program at Utrecht University. He opted for Utrecht instead of the much closer Leiden, because his uncle was a professor there and he wanted to attend his lectures. Because he was so focused on science, his father insisted that he join the Utrechtsch Studenten Corps, a student association, in the hope that he would do something else besides studying. This worked to some extent; during his studies he was a coxswain with their rowing club "Triton" and organized a national congress for science students with their science discussion club "Christiaan Huygens".

In the course of his studies he decided he wanted to go into what he perceived as the heart of theoretical physics, elementary particles. His uncle had grown to dislike the subject and in particular its practitioners, so when it became time to write his doctoraalscriptie (former name of the Dutch equivalent of a master's thesis) in 1968, 't Hooft turned to the newly appointed professor Martinus Veltman, who specialized in Yang–Mills theory, a relatively fringe subject at the time because it was thought that these could not be renormalized. His assignment was to study the Adler–Bell–Jackiw anomaly, a mismatch in the theory of the decay of neutral pions; formal arguments forbid the decay into photons, whereas practical calculations and experiments showed that this was the primary form of decay. The resolution of the problem was completely unknown at the time, and 't Hooft was unable to provide one.

In 1969, 't Hooft started on his doctoral research with Martinus Veltman as his advisor. He would work on the same subject Veltman was working on, the renormalization of Yang–Mills theories. In 1971 his first paper was published.[3] In it he showed how to renormalize massless Yang–Mills fields, and was able to derive relations between amplitudes, which would be generalized by Andrei Slavnov and John C. Taylor, and become known as the Slavnov–Taylor identities.

The world took little notice, but Veltman was excited because he saw that the problem he had been working on was solved. A period of intense collaboration followed in which they developed the technique of dimensional regularization. Soon 't Hooft's second paper was ready to be published,[4] in which he showed that Yang–Mills theories with massive fields due to spontaneous symmetry breaking could be renormalized. This paper earned them worldwide recognition, and would ultimately earn the pair the 1999 Nobel Prize in Physics.

These two papers formed the basis of 't Hooft's dissertation, The Renormalization procedure for Yang–Mills Fields, and he obtained his PhD degree in 1972. In the same year he married his wife, Albertha A. Schik, a student of medicine in Utrecht.[2]

Career

 
Gerard 't Hooft at Harvard

After obtaining his doctorate 't Hooft went to CERN in Geneva, where he had a fellowship. He further refined his methods for Yang–Mills theories with Veltman (who went back to Geneva). In this time he became interested in the possibility that the strong interaction could be described as a massless Yang–Mills theory, i.e. one of a type that he had just proved to be renormalizable and hence be susceptible to detailed calculation and comparison with experiment.

According to 't Hooft's calculations, this type of theory possessed just the right kind of scaling properties (asymptotic freedom) that this theory should have according to deep inelastic scattering experiments. This was contrary to popular perception of Yang–Mills theories at the time, that like gravitation and electrodynamics, their intensity should decrease with increasing distance between the interacting particles; such conventional behaviour with distance was unable to explain the results of deep inelastic scattering, whereas 't Hooft's calculations could.

When 't Hooft mentioned his results at a small conference at Marseilles in 1972, Kurt Symanzik urged him to publish this result;[2] but 't Hooft did not, and the result was eventually rediscovered and published by Hugh David Politzer, David Gross, and Frank Wilczek in 1973, which led to their earning the 2004 Nobel Prize in Physics.[5][6]

In 1974, 't Hooft returned to Utrecht where he became assistant professor. In 1976, he was invited for a guest position at Stanford and a position at Harvard as Morris Loeb lecturer. His eldest daughter, Saskia Anne, was born in Boston, while his second daughter, Ellen Marga, was born in 1978 after he returned to Utrecht, where he was made full professor.[2] In the academic year 1987-1988 't Hooft spent a sabbatical in the Boston University Physics Department along with Howard Georgi, Robert Jaffe and others arranged by the then new Department chair Lawrence Sulak.

In 2007 't Hooft became editor-in-chief for Foundations of Physics, where he sought to distance the journal from the controversy of ECE theory.[7] 't Hooft held the position until 2016.

On July 1, 2011 he was appointed Distinguished professor by Utrecht University.[8]

Honors

In 1999 't Hooft shared the Nobel prize in Physics with his thesis adviser Veltman for "elucidating the quantum structure of the electroweak interactions in physics".[9] Before that time his work had already been recognized by other notable awards. In 1981, he was awarded the Wolf Prize,[10] possibly the most prestigious prize in physics after the Nobel prize. Five years later he received the Lorentz Medal, awarded every four years in recognition of the most important contributions in theoretical physics.[11] In 1995, he was one of the first recipients of the Spinozapremie, the highest award available to scientists in the Netherlands.[12] In the same year he was also honoured with a Franklin Medal.[13] In 2000, 't Hooft received the Golden Plate Award of the American Academy of Achievement.[14]

Since his Nobel Prize, 't Hooft has received a slew of awards, honorary doctorates and honorary professorships.[15] He was knighted commander in the Order of the Netherlands Lion, and officer in the French Legion of Honor. The asteroid 9491 Thooft has been named in his honor,[16] and he has written a constitution for its future inhabitants.[17]

He is a member of the Royal Netherlands Academy of Arts and Sciences (KNAW) since 1982,[18] where he was made academy professor in 2003.[19] He is also a foreign member of many other science academies, including the French Académie des Sciences, the American National Academy of Sciences and American Academy of Arts and Sciences and the Britain and Ireland based Institute of Physics.[15]

't Hooft has appeared in season 3 of Through the Wormhole with Morgan Freeman.

Research

't Hooft's research interest can be divided in three main directions: 'gauge theories in elementary particle physics', 'quantum gravity and black holes', and 'foundational aspects of quantum mechanics'.[20]

Gauge theories in elementary particle physics

't Hooft is most famous for his contributions to the development of gauge theories in particle physics. The best known of these is the proof in his PhD thesis that Yang–Mills theories are renormalizable, for which he shared the 1999 Nobel Prize in Physics. For this proof he introduced (with his adviser Veltman) the technique of dimensional regularization.

After his PhD, he became interested in the role of gauge theories in the strong interaction,[2] the leading theory of which is called quantum chromodynamics or QCD. Much of his research focused on the problem of color confinement in QCD, i.e. the observational fact that only color neutral particles are observed at low energies. This led him to the discovery that SU(N) gauge theories simplify in the large N limit,[21] a fact which has proved important in the examination of the conjectured correspondence between string theories in an Anti-de Sitter space and conformal field theories in one lower dimension. By solving the theory in one space and one time dimension, 't Hooft was able to derive a formula for the masses of mesons.[22]

He also studied the role of so-called instanton contributions in QCD. His calculation showed that these contributions lead to an interaction between light quarks at low energies not present in the normal theory.[23] Studying instanton solutions of Yang–Mills theories, 't Hooft discovered that spontaneously breaking a theory with SU(N) symmetry to a U(1) symmetry will lead to the existence of magnetic monopoles.[24] These monopoles are called 't Hooft–Polyakov monopoles, after Alexander Polyakov, who independently obtained the same result.[25]

As another piece in the color confinement puzzle 't Hooft introduced 't Hooft loops, which are the magnetic dual of Wilson loops.[26] Using these operators he was able to classify different phases of QCD, which form the basis of the QCD phase diagram.

In 1986, he was finally able to show that instanton contributions solve the Adler–Bell–Jackiw anomaly, the topic of his master's thesis.[27]

Quantum gravity and black holes

When Veltman and 't Hooft moved to CERN after 't Hooft obtained his PhD, Veltman's attention was drawn to the possibility of using their dimensional regularization techniques to the problem of quantizing gravity. Although it was known that perturbative quantum gravity was not completely renormalizible, they felt important lessons were to be learned by studying the formal renormalization of the theory order by order. This work would be continued by Stanley Deser and another PhD student of Veltman, Peter van Nieuwenhuizen, who later found patterns in the renormalization counter terms, which led to the discovery of supergravity.[2]

In the 1980s, 't Hooft's attention was drawn to the subject of gravity in 3 spacetime dimensions. Together with Deser and Jackiw he published an article in 1984 describing the dynamics of flat space where the only local degrees of freedom were propagating point defects.[28] His attention returned to this model at various points in time, showing that Gott pairs would not cause causality violating timelike loops,[29] and showing how the model could be quantized.[30] More recently he proposed generalizing this piecewise flat model of gravity to 4 spacetime dimensions.[31]

With Stephen Hawking's discovery of Hawking radiation of black holes, it appeared that the evaporation of these objects violated a fundamental property of quantum mechanics, unitarity. 't Hooft refused to accept this problem, known as the black hole information paradox, and assumed that this must be the result of the semi-classical treatment of Hawking, and that it should not appear in a full theory of quantum gravity. He proposed that it might be possible to study some of the properties of such a theory, by assuming that such a theory was unitary.

Using this approach he has argued that near a black hole, quantum fields could be described by a theory in a lower dimension.[32] This led to the introduction of the holographic principle by him and Leonard Susskind.[33]

Fundamental aspects of quantum mechanics

't Hooft has "deviating views on the physical interpretation of quantum theory".[20] He believes that there could be a deterministic explanation underlying quantum mechanics.[34] Using a speculative model he has argued that such a theory could avoid the usual Bell inequality arguments that would disallow such a local hidden-variable theory.[35] In 2016 he published a book length exposition of his ideas[36] which, according to 't Hooft, has encountered mixed reactions.[37]

Popular publications

  • 't Hooft, Gerard (2008). Playing with Planets. doi:10.1142/6702. ISBN 978-981-279-307-2.
  • 't Hooft, Gerard (1996). In Search of the Ultimate Building Blocks. doi:10.1017/CBO9781107340855. ISBN 9780521550833.
  • 't Hooft, Gerard (2014). Time in Powers of Ten. doi:10.1142/8786. ISBN 978-981-4489-80-5.

Academic publications

  • 't Hooft, Gerard (2016). The Cellular Automaton Interpretation of Quantum Mechanics (Fundamental Theories of Physics, 185). Fundamental Theories of Physics. Vol. 185. doi:10.1007/978-3-319-41285-6. ISBN 978-3-319-41284-9. S2CID 7779840.


See also

References

  1. ^ "Gerardus 't Hooft - Facts". nobelprize.org. Retrieved 20 August 2021.
  2. ^ a b c d e f g h 't Hooft, G. (1999). "Gerardus 't Hooft — Autobiography". Nobel web. Retrieved 2010-10-06.
  3. ^ 't Hooft, G. (1971). "Renormalization of massless Yang–Mills fields". Nuclear Physics B. 33 (1): 173–177. Bibcode:1971NuPhB..33..173T. doi:10.1016/0550-3213(71)90395-6.
  4. ^ 't Hooft, G. (1971). "Renormalizable Lagrangians for massive Yang–Mills fields". Nuclear Physics B. 35 (1): 167–188. Bibcode:1971NuPhB..35..167T. doi:10.1016/0550-3213(71)90139-8. hdl:1874/4733.
  5. ^ "The Nobel Prize in Physics 2004". Nobel Web. 2004. Retrieved 2010-10-24.
  6. ^ Politzer, H. David (2004). "The Dilemma of Attribution" (PDF). Proceedings of the National Academy of Sciences of the United States of America. Nobel Web. 102 (22): 7789–93. doi:10.1073/pnas.0501644102. PMC 1142376. PMID 15911758. Retrieved 2010-10-24.
  7. ^ ’t Hooft, Gerard (2007). "Editorial note". Foundations of Physics. 38 (1): 1–2. Bibcode:2008FoPh...38....1T. doi:10.1007/s10701-007-9187-8. ISSN 0015-9018. S2CID 189843269.
  8. ^ . Utrecht University. Archived from the original on 2012-04-14. Retrieved 2012-04-19.
  9. ^ "The Nobel Prize in Physics 1999". Nobel web.
  10. ^ . Wolf Foundation. Archived from the original on 2011-09-27.
  11. ^ "Lorentz medal". Leiden University.
  12. ^ . Netherlands Organisation for Scientific Research. 3 September 2014. Archived from the original on 2015-06-29. Retrieved 2016-01-30.
  13. ^ . The Franklin Institute. Archived from the original on 2010-06-01.
  14. ^ "Golden Plate Awardees of the American Academy of Achievement". www.achievement.org. American Academy of Achievement.
  15. ^ a b "Curriculum Vitae Gerard 't Hooft". G. 't Hooft.
  16. ^ "JPL Small-Body Database Browser". NASA.
  17. ^ "9491 THOOFT — Constitution and Bylaws". G. 't Hooft.
  18. ^ . Royal Netherlands Academy of Arts and Sciences. Archived from the original on 2020-07-23. Retrieved 2015-07-17.
  19. ^ . Royal Netherlands Academy of Arts and Sciences. Archived from the original on 2010-11-24.
  20. ^ a b 't Hooft, G. "Gerard 't Hooft". Retrieved 2010-10-24.
  21. ^ 't Hooft, G. (1974). "A planar diagram theory for strong interactions". Nuclear Physics B. 72 (3): 461–470. Bibcode:1974NuPhB..72..461T. doi:10.1016/0550-3213(74)90154-0.
  22. ^ 't Hooft, G. (1974). "A two-dimensional model for mesons". Nuclear Physics B. 75 (3): 461–863. Bibcode:1974NuPhB..75..461T. doi:10.1016/0550-3213(74)90088-1.
  23. ^ 't Hooft, G. (1976). "Computation of the quantum effects due to a four-dimensional pseudoparticle". Physical Review D. 14 (12): 3432–3450. Bibcode:1976PhRvD..14.3432T. doi:10.1103/PhysRevD.14.3432.
  24. ^ 't Hooft, G. (1974). "Magnetic monopoles in unified gauge theories". Nuclear Physics B. 79 (2): 276–284. Bibcode:1974NuPhB..79..276T. doi:10.1016/0550-3213(74)90486-6. hdl:1874/4686.
  25. ^ Polyakov, A.M. (1974). . Journal of Experimental and Theoretical Physics Letters. 20: 194. Bibcode:1974JETPL..20..194P. Archived from the original on 2019-07-09. Retrieved 2018-08-11.
  26. ^ 't Hooft, G. (1978). "On the phase transition towards permanent quark confinement". Nuclear Physics B. 138 (1): 1–2. Bibcode:1978NuPhB.138....1T. doi:10.1016/0550-3213(78)90153-0.
  27. ^ 't Hooft, G. (1986). "How instantons solve the U(1) problem". Physics Reports. 142 (6): 357–712. Bibcode:1986PhR...142..357T. doi:10.1016/0370-1573(86)90117-1.
  28. ^ Deser, S.; Jackiw, R.; 't Hooft, G. (1984). "Three-dimensional Einstein gravity: Dynamics of flat space". Annals of Physics. 152 (1): 220. Bibcode:1984AnPhy.152..220D. doi:10.1016/0003-4916(84)90085-X. hdl:1874/4772.
  29. ^ 't Hooft, G. (1992). "Causality in (2+1)-dimensional gravity". Classical and Quantum Gravity. 9 (5): 1335–1348. Bibcode:1992CQGra...9.1335T. doi:10.1088/0264-9381/9/5/015. hdl:1874/4627. S2CID 250821900.
  30. ^ 't Hooft, G. (1993). "Canonical quantization of gravitating point particles in 2+1 dimensions". Classical and Quantum Gravity. 10 (8): 1653–1664. arXiv:gr-qc/9305008. Bibcode:1993CQGra..10.1653T. doi:10.1088/0264-9381/10/8/022. S2CID 119521701.
  31. ^ 't Hooft, G. (2008). "A Locally Finite Model for Gravity". Foundations of Physics. 38 (8): 733–757. arXiv:0804.0328. Bibcode:2008FoPh...38..733T. doi:10.1007/s10701-008-9231-3. S2CID 189844967.
  32. ^ Stephens, C. R.; 't Hooft, G.; Whiting, B. F. (1994). "Black hole evaporation without information loss". Classical and Quantum Gravity. 11 (3): 621–648. arXiv:gr-qc/9310006. Bibcode:1994CQGra..11..621S. doi:10.1088/0264-9381/11/3/014. S2CID 15489828.
  33. ^ Susskind, L. (1995). "The world as a hologram". Journal of Mathematical Physics. 36 (11): 6377–6396. arXiv:hep-th/9409089. Bibcode:1995JMP....36.6377S. doi:10.1063/1.531249. S2CID 17316840.
  34. ^ 't Hooft, G. (2007). "A mathematical theory for deterministic quantum mechanics". Journal of Physics: Conference Series. 67 (1): 012015. arXiv:quant-ph/0604008. Bibcode:2007JPhCS..67a2015T. doi:10.1088/1742-6596/67/1/012015. S2CID 15908445.
  35. ^ Gerard 't Hooft (2009). "Entangled quantum states in a local deterministic theory". arXiv:0908.3408 [quant-ph].
  36. ^ Gerard 't Hooft, 2016, The Cellular Automaton Interpretation of Quantum Mechanics, Springer International Publishing, DOI 10.1007/978-3-319-41285-6, Open access-[1]
  37. ^ Baldwin, Melinda (2017-07-11). "Q&A: Gerard 't Hooft on the future of quantum mechanics". Physics Today. doi:10.1063/pt.6.4.20170711a.

External links

  • Gerard 't Hooft (homepage)
  • How To Become a Good Theoretical Physicist
  • Gerard 't Hooft on Nobelprize.org   including the Nobel Lecture A Confrontation with Infinity
  • Publications from Google Scholar
  • Publications on the arXiv
  • TVO.org video - Gerard t'Hooft lectures on Science Fiction and Reality Lecture delivered at the Perimeter Institute in Waterloo, Ontario, Canada on May 7, 2008
  • Gerard 't Hooft on INSPIRE-HEP  

gerard, hooft, this, dutch, name, family, name, hooft, hooft, gerardus, gerard, hooft, dutch, ˈɣeːrɑrt, ˈɦoːft, born, july, 1946, dutch, theoretical, physicist, professor, utrecht, university, netherlands, shared, 1999, nobel, prize, physics, with, thesis, adv. This is a Dutch name the family name is t Hooft not Hooft Gerardus Gerard t Hooft Dutch ˈɣeːrɑrt et ˈɦoːft born July 5 1946 is a Dutch theoretical physicist and professor at Utrecht University the Netherlands He shared the 1999 Nobel Prize in Physics with his thesis advisor Martinus J G Veltman for elucidating the quantum structure of electroweak interactions Gerard t Hooft t Hooft in November 2008Born 1946 07 05 July 5 1946 age 76 Den Helder NetherlandsNationalityDutchAlma materUtrecht UniversityKnown forQuantum field theoryQuantum gravity t Hooft condition t Hooft Polyakov monopole t Hooft symbol t Hooft loopFeynman t Hooft gaugeBlack hole complementarityMinimal subtraction schemeHolographic principleRenormalization of Yang Mills theoryDimensional regularizationRenormalon1 N expansionAwardsHeineman Prize 1979 Wolf Prize 1981 Lorentz Medal 1986 Spinoza Prize 1995 Franklin Medal 1995 Nobel Prize in Physics 1999 High Energy and Particle Physics Prize 1999 Lomonosov Gold Medal 2010 Scientific careerFieldsTheoretical physicsInstitutionsUtrecht UniversityDoctoral advisorMartinus J G VeltmanDoctoral studentsRobbert DijkgraafHerman VerlindeMax WellingHis work concentrates on gauge theory black holes quantum gravity and fundamental aspects of quantum mechanics His contributions to physics include a proof that gauge theories are renormalizable dimensional regularization and the holographic principle Contents 1 Personal life 2 Biography 2 1 Early life 2 2 Education 2 3 Career 3 Honors 4 Research 4 1 Gauge theories in elementary particle physics 4 2 Quantum gravity and black holes 4 3 Fundamental aspects of quantum mechanics 5 Popular publications 6 Academic publications 7 See also 8 References 9 External linksPersonal life EditHe is married to Albertha Schik Betteke and has two daughters Biography EditEarly life Edit Gerard t Hooft was born in Den Helder on July 5 1946 1 but grew up in The Hague He was the middle child of a family of three He comes from a family of scholars His great uncle was Nobel prize laureate Frits Zernike and his grandmother was married to Pieter Nicolaas van Kampen a professor of zoology at Leiden University His uncle Nico van Kampen was an emeritus professor of theoretical physics at Utrecht University and his mother married a maritime engineer 2 Following his family s footsteps he showed interest in science at an early age When his primary school teacher asked him what he wanted to be when he grew up he replied a man who knows everything 2 After primary school Gerard attended the Dalton Lyceum a school that applied the ideas of the Dalton Plan an educational method that suited him well He excelled at science and mathematics courses At the age of sixteen he won a silver medal in the second Dutch Math Olympiad 2 Education Edit After Gerard t Hooft passed his high school exams in 1964 he enrolled in the physics program at Utrecht University He opted for Utrecht instead of the much closer Leiden because his uncle was a professor there and he wanted to attend his lectures Because he was so focused on science his father insisted that he join the Utrechtsch Studenten Corps a student association in the hope that he would do something else besides studying This worked to some extent during his studies he was a coxswain with their rowing club Triton and organized a national congress for science students with their science discussion club Christiaan Huygens In the course of his studies he decided he wanted to go into what he perceived as the heart of theoretical physics elementary particles His uncle had grown to dislike the subject and in particular its practitioners so when it became time to write his doctoraalscriptie former name of the Dutch equivalent of a master s thesis in 1968 t Hooft turned to the newly appointed professor Martinus Veltman who specialized in Yang Mills theory a relatively fringe subject at the time because it was thought that these could not be renormalized His assignment was to study the Adler Bell Jackiw anomaly a mismatch in the theory of the decay of neutral pions formal arguments forbid the decay into photons whereas practical calculations and experiments showed that this was the primary form of decay The resolution of the problem was completely unknown at the time and t Hooft was unable to provide one In 1969 t Hooft started on his doctoral research with Martinus Veltman as his advisor He would work on the same subject Veltman was working on the renormalization of Yang Mills theories In 1971 his first paper was published 3 In it he showed how to renormalize massless Yang Mills fields and was able to derive relations between amplitudes which would be generalized by Andrei Slavnov and John C Taylor and become known as the Slavnov Taylor identities The world took little notice but Veltman was excited because he saw that the problem he had been working on was solved A period of intense collaboration followed in which they developed the technique of dimensional regularization Soon t Hooft s second paper was ready to be published 4 in which he showed that Yang Mills theories with massive fields due to spontaneous symmetry breaking could be renormalized This paper earned them worldwide recognition and would ultimately earn the pair the 1999 Nobel Prize in Physics These two papers formed the basis of t Hooft s dissertation The Renormalization procedure for Yang Mills Fields and he obtained his PhD degree in 1972 In the same year he married his wife Albertha A Schik a student of medicine in Utrecht 2 Career Edit Gerard t Hooft at Harvard After obtaining his doctorate t Hooft went to CERN in Geneva where he had a fellowship He further refined his methods for Yang Mills theories with Veltman who went back to Geneva In this time he became interested in the possibility that the strong interaction could be described as a massless Yang Mills theory i e one of a type that he had just proved to be renormalizable and hence be susceptible to detailed calculation and comparison with experiment According to t Hooft s calculations this type of theory possessed just the right kind of scaling properties asymptotic freedom that this theory should have according to deep inelastic scattering experiments This was contrary to popular perception of Yang Mills theories at the time that like gravitation and electrodynamics their intensity should decrease with increasing distance between the interacting particles such conventional behaviour with distance was unable to explain the results of deep inelastic scattering whereas t Hooft s calculations could When t Hooft mentioned his results at a small conference at Marseilles in 1972 Kurt Symanzik urged him to publish this result 2 but t Hooft did not and the result was eventually rediscovered and published by Hugh David Politzer David Gross and Frank Wilczek in 1973 which led to their earning the 2004 Nobel Prize in Physics 5 6 In 1974 t Hooft returned to Utrecht where he became assistant professor In 1976 he was invited for a guest position at Stanford and a position at Harvard as Morris Loeb lecturer His eldest daughter Saskia Anne was born in Boston while his second daughter Ellen Marga was born in 1978 after he returned to Utrecht where he was made full professor 2 In the academic year 1987 1988 t Hooft spent a sabbatical in the Boston University Physics Department along with Howard Georgi Robert Jaffe and others arranged by the then new Department chair Lawrence Sulak In 2007 t Hooft became editor in chief for Foundations of Physics where he sought to distance the journal from the controversy of ECE theory 7 t Hooft held the position until 2016 On July 1 2011 he was appointed Distinguished professor by Utrecht University 8 Honors EditIn 1999 t Hooft shared the Nobel prize in Physics with his thesis adviser Veltman for elucidating the quantum structure of the electroweak interactions in physics 9 Before that time his work had already been recognized by other notable awards In 1981 he was awarded the Wolf Prize 10 possibly the most prestigious prize in physics after the Nobel prize Five years later he received the Lorentz Medal awarded every four years in recognition of the most important contributions in theoretical physics 11 In 1995 he was one of the first recipients of the Spinozapremie the highest award available to scientists in the Netherlands 12 In the same year he was also honoured with a Franklin Medal 13 In 2000 t Hooft received the Golden Plate Award of the American Academy of Achievement 14 Since his Nobel Prize t Hooft has received a slew of awards honorary doctorates and honorary professorships 15 He was knighted commander in the Order of the Netherlands Lion and officer in the French Legion of Honor The asteroid 9491 Thooft has been named in his honor 16 and he has written a constitution for its future inhabitants 17 He is a member of the Royal Netherlands Academy of Arts and Sciences KNAW since 1982 18 where he was made academy professor in 2003 19 He is also a foreign member of many other science academies including the French Academie des Sciences the American National Academy of Sciences and American Academy of Arts and Sciences and the Britain and Ireland based Institute of Physics 15 t Hooft has appeared in season 3 of Through the Wormhole with Morgan Freeman Research Edit t Hooft s research interest can be divided in three main directions gauge theories in elementary particle physics quantum gravity and black holes and foundational aspects of quantum mechanics 20 Gauge theories in elementary particle physics Edit t Hooft is most famous for his contributions to the development of gauge theories in particle physics The best known of these is the proof in his PhD thesis that Yang Mills theories are renormalizable for which he shared the 1999 Nobel Prize in Physics For this proof he introduced with his adviser Veltman the technique of dimensional regularization After his PhD he became interested in the role of gauge theories in the strong interaction 2 the leading theory of which is called quantum chromodynamics or QCD Much of his research focused on the problem of color confinement in QCD i e the observational fact that only color neutral particles are observed at low energies This led him to the discovery that SU N gauge theories simplify in the large N limit 21 a fact which has proved important in the examination of the conjectured correspondence between string theories in an Anti de Sitter space and conformal field theories in one lower dimension By solving the theory in one space and one time dimension t Hooft was able to derive a formula for the masses of mesons 22 He also studied the role of so called instanton contributions in QCD His calculation showed that these contributions lead to an interaction between light quarks at low energies not present in the normal theory 23 Studying instanton solutions of Yang Mills theories t Hooft discovered that spontaneously breaking a theory with SU N symmetry to a U 1 symmetry will lead to the existence of magnetic monopoles 24 These monopoles are called t Hooft Polyakov monopoles after Alexander Polyakov who independently obtained the same result 25 As another piece in the color confinement puzzle t Hooft introduced t Hooft loops which are the magnetic dual of Wilson loops 26 Using these operators he was able to classify different phases of QCD which form the basis of the QCD phase diagram In 1986 he was finally able to show that instanton contributions solve the Adler Bell Jackiw anomaly the topic of his master s thesis 27 Quantum gravity and black holes Edit When Veltman and t Hooft moved to CERN after t Hooft obtained his PhD Veltman s attention was drawn to the possibility of using their dimensional regularization techniques to the problem of quantizing gravity Although it was known that perturbative quantum gravity was not completely renormalizible they felt important lessons were to be learned by studying the formal renormalization of the theory order by order This work would be continued by Stanley Deser and another PhD student of Veltman Peter van Nieuwenhuizen who later found patterns in the renormalization counter terms which led to the discovery of supergravity 2 In the 1980s t Hooft s attention was drawn to the subject of gravity in 3 spacetime dimensions Together with Deser and Jackiw he published an article in 1984 describing the dynamics of flat space where the only local degrees of freedom were propagating point defects 28 His attention returned to this model at various points in time showing that Gott pairs would not cause causality violating timelike loops 29 and showing how the model could be quantized 30 More recently he proposed generalizing this piecewise flat model of gravity to 4 spacetime dimensions 31 With Stephen Hawking s discovery of Hawking radiation of black holes it appeared that the evaporation of these objects violated a fundamental property of quantum mechanics unitarity t Hooft refused to accept this problem known as the black hole information paradox and assumed that this must be the result of the semi classical treatment of Hawking and that it should not appear in a full theory of quantum gravity He proposed that it might be possible to study some of the properties of such a theory by assuming that such a theory was unitary Using this approach he has argued that near a black hole quantum fields could be described by a theory in a lower dimension 32 This led to the introduction of the holographic principle by him and Leonard Susskind 33 Fundamental aspects of quantum mechanics Edit t Hooft has deviating views on the physical interpretation of quantum theory 20 He believes that there could be a deterministic explanation underlying quantum mechanics 34 Using a speculative model he has argued that such a theory could avoid the usual Bell inequality arguments that would disallow such a local hidden variable theory 35 In 2016 he published a book length exposition of his ideas 36 which according to t Hooft has encountered mixed reactions 37 Popular publications Edit t Hooft Gerard 2008 Playing with Planets doi 10 1142 6702 ISBN 978 981 279 307 2 t Hooft Gerard 1996 In Search of the Ultimate Building Blocks doi 10 1017 CBO9781107340855 ISBN 9780521550833 t Hooft Gerard 2014 Time in Powers of Ten doi 10 1142 8786 ISBN 978 981 4489 80 5 Academic publications Edit t Hooft Gerard 2016 The Cellular Automaton Interpretation of Quantum Mechanics Fundamental Theories of Physics 185 Fundamental Theories of Physics Vol 185 doi 10 1007 978 3 319 41285 6 ISBN 978 3 319 41284 9 S2CID 7779840 See also EditAsymptotic freedom Center vortex Naturalness physics Pauli Villars regularization Slavnov Taylor identities Superdeterminism Mars One Gerard t Hooft is a main supporter of the project References Edit Gerardus t Hooft Facts nobelprize org Retrieved 20 August 2021 a b c d e f g h t Hooft G 1999 Gerardus t Hooft Autobiography Nobel web Retrieved 2010 10 06 t Hooft G 1971 Renormalization of massless Yang Mills fields Nuclear Physics B 33 1 173 177 Bibcode 1971NuPhB 33 173T doi 10 1016 0550 3213 71 90395 6 t Hooft G 1971 Renormalizable Lagrangians for massive Yang Mills fields Nuclear Physics B 35 1 167 188 Bibcode 1971NuPhB 35 167T doi 10 1016 0550 3213 71 90139 8 hdl 1874 4733 The Nobel Prize in Physics 2004 Nobel Web 2004 Retrieved 2010 10 24 Politzer H David 2004 The Dilemma of Attribution PDF Proceedings of the National Academy of Sciences of the United States of America Nobel Web 102 22 7789 93 doi 10 1073 pnas 0501644102 PMC 1142376 PMID 15911758 Retrieved 2010 10 24 t Hooft Gerard 2007 Editorial note Foundations of Physics 38 1 1 2 Bibcode 2008FoPh 38 1T doi 10 1007 s10701 007 9187 8 ISSN 0015 9018 S2CID 189843269 Prof dr Gerard t Hooft has been appointed Distinguished Professor Utrecht University Archived from the original on 2012 04 14 Retrieved 2012 04 19 The Nobel Prize in Physics 1999 Nobel web The 1981 Wolf Foundation Prize in Physics Wolf Foundation Archived from the original on 2011 09 27 Lorentz medal Leiden University NWO Spinoza Prize 1995 Netherlands Organisation for Scientific Research 3 September 2014 Archived from the original on 2015 06 29 Retrieved 2016 01 30 Franklin Laureate Database The Franklin Institute Archived from the original on 2010 06 01 Golden Plate Awardees of the American Academy of Achievement www achievement org American Academy of Achievement a b Curriculum Vitae Gerard t Hooft G t Hooft JPL Small Body Database Browser NASA 9491 THOOFT Constitution and Bylaws G t Hooft Gerard t Hooft Royal Netherlands Academy of Arts and Sciences Archived from the original on 2020 07 23 Retrieved 2015 07 17 Academy Professorships Programme 2003 Royal Netherlands Academy of Arts and Sciences Archived from the original on 2010 11 24 a b t Hooft G Gerard t Hooft Retrieved 2010 10 24 t Hooft G 1974 A planar diagram theory for strong interactions Nuclear Physics B 72 3 461 470 Bibcode 1974NuPhB 72 461T doi 10 1016 0550 3213 74 90154 0 t Hooft G 1974 A two dimensional model for mesons Nuclear Physics B 75 3 461 863 Bibcode 1974NuPhB 75 461T doi 10 1016 0550 3213 74 90088 1 t Hooft G 1976 Computation of the quantum effects due to a four dimensional pseudoparticle Physical Review D 14 12 3432 3450 Bibcode 1976PhRvD 14 3432T doi 10 1103 PhysRevD 14 3432 t Hooft G 1974 Magnetic monopoles in unified gauge theories Nuclear Physics B 79 2 276 284 Bibcode 1974NuPhB 79 276T doi 10 1016 0550 3213 74 90486 6 hdl 1874 4686 Polyakov A M 1974 Particle spectrum in quantum field theory Journal of Experimental and Theoretical Physics Letters 20 194 Bibcode 1974JETPL 20 194P Archived from the original on 2019 07 09 Retrieved 2018 08 11 t Hooft G 1978 On the phase transition towards permanent quark confinement Nuclear Physics B 138 1 1 2 Bibcode 1978NuPhB 138 1T doi 10 1016 0550 3213 78 90153 0 t Hooft G 1986 How instantons solve the U 1 problem Physics Reports 142 6 357 712 Bibcode 1986PhR 142 357T doi 10 1016 0370 1573 86 90117 1 Deser S Jackiw R t Hooft G 1984 Three dimensional Einstein gravity Dynamics of flat space Annals of Physics 152 1 220 Bibcode 1984AnPhy 152 220D doi 10 1016 0003 4916 84 90085 X hdl 1874 4772 t Hooft G 1992 Causality in 2 1 dimensional gravity Classical and Quantum Gravity 9 5 1335 1348 Bibcode 1992CQGra 9 1335T doi 10 1088 0264 9381 9 5 015 hdl 1874 4627 S2CID 250821900 t Hooft G 1993 Canonical quantization of gravitating point particles in 2 1 dimensions Classical and Quantum Gravity 10 8 1653 1664 arXiv gr qc 9305008 Bibcode 1993CQGra 10 1653T doi 10 1088 0264 9381 10 8 022 S2CID 119521701 t Hooft G 2008 A Locally Finite Model for Gravity Foundations of Physics 38 8 733 757 arXiv 0804 0328 Bibcode 2008FoPh 38 733T doi 10 1007 s10701 008 9231 3 S2CID 189844967 Stephens C R t Hooft G Whiting B F 1994 Black hole evaporation without information loss Classical and Quantum Gravity 11 3 621 648 arXiv gr qc 9310006 Bibcode 1994CQGra 11 621S doi 10 1088 0264 9381 11 3 014 S2CID 15489828 Susskind L 1995 The world as a hologram Journal of Mathematical Physics 36 11 6377 6396 arXiv hep th 9409089 Bibcode 1995JMP 36 6377S doi 10 1063 1 531249 S2CID 17316840 t Hooft G 2007 A mathematical theory for deterministic quantum mechanics Journal of Physics Conference Series 67 1 012015 arXiv quant ph 0604008 Bibcode 2007JPhCS 67a2015T doi 10 1088 1742 6596 67 1 012015 S2CID 15908445 Gerard t Hooft 2009 Entangled quantum states in a local deterministic theory arXiv 0908 3408 quant ph Gerard t Hooft 2016 The Cellular Automaton Interpretation of Quantum Mechanics Springer International Publishing DOI 10 1007 978 3 319 41285 6 Open access 1 Baldwin Melinda 2017 07 11 Q amp A Gerard t Hooft on the future of quantum mechanics Physics Today doi 10 1063 pt 6 4 20170711a External links Edit Wikimedia Commons has media related to Gerardus t Hooft Wikiquote has quotations related to Gerardus t Hooft Gerard t Hooft homepage How To Become a Good Theoretical Physicist Gerard t Hooft on Nobelprize org including the Nobel Lecture A Confrontation with Infinity Publications from Google Scholar Publications on the arXiv TVO org video Gerard t Hooft lectures on Science Fiction and Reality Lecture delivered at the Perimeter Institute in Waterloo Ontario Canada on May 7 2008 Gerard t Hooft on INSPIRE HEP Retrieved from https en wikipedia org w index php title Gerard 27t Hooft amp oldid 1152718851, wikipedia, wiki, book, books, library,

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