H. J. Crawford
University of California, Berkeley
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Featured researches published by H. J. Crawford.
Nature | 2017
L. Adamczyk; J. K. Adkins; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; N. N. Ajitanand; I. Alekseev; D. M. Anderson; R. Aoyama; A. Aparin; D. Arkhipkin; E. C. Aschenauer; M. U. Ashraf; A. Attri; G. S. Averichev; X. Bai; Bairathi; Arabinda Behera; R. Bellwied; A. Bhasin; Ashok Kumar Bhati; P. Bhattarai; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; J. Bouchet; J. D. Brandenburg; A. V. Brandin; D. D. Brown
The extreme energy densities generated by ultra-relativistic collisions between heavy atomic nuclei produce a state of matter that behaves surprisingly like a fluid, with exceptionally high temperature and low viscosity. Non-central collisions have angular momenta of the order of 1,000ћ, and the resulting fluid may have a strong vortical structure that must be understood to describe the fluid properly. The vortical structure is also of particular interest because the restoration of fundamental symmetries of quantum chromodynamics is expected to produce novel physical effects in the presence of strong vorticity. However, no experimental indications of fluid vorticity in heavy ion collisions have yet been found. Since vorticity represents a local rotational structure of the fluid, spin–orbit coupling can lead to preferential orientation of particle spins along the direction of rotation. Here we present measurements of an alignment between the global angular momentum of a non-central collision and the spin of emitted particles (in this case the collision occurs between gold nuclei and produces Λ baryons), revealing that the fluid produced in heavy ion collisions is the most vortical system so far observed. (At high energies, this fluid is a quark–gluon plasma.) We find that Λ and hyperons show a positive polarization of the order of a few per cent, consistent with some hydrodynamic predictions. (A hyperon is a particle composed of three quarks, at least one of which is a strange quark; the remainder are up and down quarks, found in protons and neutrons.) A previous measurement that reported a null result, that is, zero polarization, at higher collision energies is seen to be consistent with the trend of our observations, though with larger statistical uncertainties. These data provide experimental access to the vortical structure of the nearly ideal liquid created in a heavy ion collision and should prove valuable in the development of hydrodynamic models that quantitatively connect observations to the theory of the strong force.The extreme temperatures and energy densities generated by ultra-relativistic collisions between heavy nuclei produce a state of matter with surprising fluid properties1. Non-central collisions have angular momentum on the order of 1000~, and the resulting fluid may have a strong vortical structure2–4 that must be understood to properly describe the fluid. It is also of particular interest because the restoration of fundamental symmetries of quantum chromodynamics is expected to produce novel physical effects in the presence of strong vorticity15. However, no experimental indications of fluid vorticity in heavy ion collisions have so far been found. Here we present the first measurement of an alignment between the angular momentum of a non-central collision and the spin of emitted particles, revealing that the fluid produced in heavy ion collisions is by far the most vortical system ever observed. We find that Λ and Λ hyperons show a positive polarization of the order of a few percent, consistent with some hydrodynamic predictions5. A previous measurement6 that reported a null result at higher collision energies is seen to be consistent with the trend of our new observations, though with larger statistical uncertainties. These data provide the first experimental access to the vortical structure of the “perfect fluid”7 created in a heavy ion collision. They should prove valuable in the development of hydrodynamic models that quantitatively connect observations to the theory of the Strong Force. Our results extend the recent discovery8 of
Physical Review C | 2017
L. Adamczyk; J. K. Adkins; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; N. N. Ajitanand; I. Alekseev; D. M. Anderson; R. Aoyama; A. Aparin; D. Arkhipkin; E. C. Aschenauer; M. U. Ashraf; A. Attri; G. S. Averichev; X. Bai; Bairathi; Arabinda Behera; R. Bellwied; A. Bhasin; Ashok Kumar Bhati; P. Bhattarai; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; J. Bouchet; J. D. Brandenburg; A. V. Brandin; D. Brown
© 2017 American Physical Society. We present measurements of bulk properties of the matter produced in Au+Au collisions at sNN=7.7,11.5,19.6,27, and 39 GeV using identified hadrons (π±, K±, p, and p) from the STAR experiment in the Beam Energy Scan (BES) Program at the Relativistic Heavy Ion Collider (RHIC). Midrapidity (|y| < 0.1) results for multiplicity densities dN/dy, average transverse momenta (pT), and particle ratios are presented. The chemical and kinetic freeze-out dynamics at these energies are discussed and presented as a function of collision centrality and energy. These results constitute the systematic measurements of bulk properties of matter formed in heavy-ion collisions over a broad range of energy (or baryon chemical potential) at RHIC.
Physics Letters B | 1987
T. Abbott; Y. Akiba; D.E. Alburger; D. Beavis; Russell Richard Betts; M. A. Bloomer; P.D. Bond; C. Chasman; Y.Y. Chu; B.A. Cole; J.B. Costales; H. J. Crawford; J.B. Cumming; R. Debbe; E. Duek; H.A. Enge; J. Engelage; S.Y. Fung; D. Greiner; L. Grodzins; S. Gushue; H. Hamagaki; O. Hansen; P. Haustein; S. Hayashi; S. Homma; H.N. Huang; Y. Ikeda; S. Katcoff; S. Kaufman
Abstract The first data from a 16O beam of total energy 232 GeV at the BNL Tandem-AGS are reported. A lead-glass array covering the laboratory pseudo-rapidity interval 1.25
Physical Review Letters | 2017
L. Adamczyk; J. K. Adkins; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; I. Alekseev; D. M. Anderson; R. Aoyama; A. Aparin; D. Arkhipkin; E. C. Aschenauer; M. U. Ashraf; A. Attri; G. S. Averichev; X. Bai; Bairathi; R. Bellwied; A. Bhasin; Ashok Kumar Bhati; P. Bhattarai; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; J. Bouchet; J. D. Brandenburg; A. V. Brandin; D. Brown; I. Bunzarov; J. M. Butterworth
We report the first di-jet transverse momentum asymmetry measurements from Au+Au and p+p collisions at RHIC. The two highest-energy back-to-back jets reconstructed from fragments with transverse momenta above 2 GeV/c display a significantly stronger momentum imbalance in heavy-ion collisions than in the p+p reference. When re-examined with correlated soft particles included, we observe that these di-jets then exhibit a unique new feature -- momentum balance is restored to that observed in p+p for a jet resolution parameter of R=0.4, while re-balancing is not attained with a smaller value of R=0.2.We report the first dijet transverse momentum asymmetry measurements from Au+Au and pp collisions at RHIC. The two highest-energy back-to-back jets reconstructed from fragments with transverse momenta above 2u2009u2009GeV/c display a significantly higher momentum imbalance in heavy-ion collisions than in the pp reference. When reexamined with correlated soft particles included, we observe that these dijets then exhibit a unique new feature-momentum balance is restored to that observed in pp for a jet resolution parameter of R=0.4, while rebalancing is not attained with a smaller value of R=0.2.
European Physical Journal C | 1988
L.P. Remsberg; M. J. Tannenbaum; T. Abbott; Y. Akiba; D.E. Alburger; D. Beavis; Russell Richard Betts; M.A. Bloomer; P.D. Bond; C. Chasman; Y.Y. Chu; B.A. Cole; J.B. Costales; H. J. Crawford; J.B. Cumming; R. Debbe; E. Duek; H. A. Enge; J. Engelage; S. Y. Fung; D. Greiner; L. Grodzins; S. Gushue; H. Hamagaki; O. Hansen; P. Haustein; S. Hayashi; S. Homma; H.Z. Huang; Y. Ikeda
The first data from a16O beam of total energy 232 GeV at the BNL Tandem-AGS are discussed. Preliminary results from a28Si beam of total energy 406 GeV are also shown. The full complement of E802, including a magnetic spectrometer, was used for the28Si measurement. A different experimental arrangement was used for16O. Comparison measurements with proton beams are presented for both configurations.
European Physical Journal C | 2005
L. C. Bland; F. Bieser; R. L. Brown; H. J. Crawford; A.A. Derevshchikov; J. L. Drachenberg; J. Engelage; L. Eun; C. A. Gagliardi; S. Heppelmann; E. G. Judd; V. I. Kravtsov; Yu. A. Matulenko; A. P. Meschanin; D. A. Morozov; L. V. Nogach; S. B. Nurushev; A. Ogawa; C. Perkins; G. Rakness; K. E. Shestermanov; A. N. Vasiliev
Abstract.Comparisons of particle production from high-energy ion collisions with next-to-leading order perturbative QCD calculations show good agreement down to moderate transverse momentum values. Distributions of azimuthal angle differences between coincident hadrons in these collisions support a partonic origin to the particle production, again down to moderate transverse momentum values. The rapidity dependence of inclusive and coincident particle production can therefore be used to probe parton distribution functions down to small momentum fractions where theory anticipates that parton saturation could be present. This paper describes how such experiments could be completed.
Physical Review C | 2016
L. Adamczyk; J. K. Adkins; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; I. Alekseev; D. M. Anderson; R. Aoyama; A. Aparin; D. Arkhipkin; E. C. Aschenauer; M. U. Ashraf; A. Attri; G. S. Averichev; X. Bai; V. Bairathi; R. Bellwied; A. Bhasin; Ashok Kumar Bhati; P. Bhattarai; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; J. Bouchet; J. D. Brandenburg; A. V. Brandin; I. Bunzarov; J. M. Butterworth; H. Caines
We present a measurement of the inclusive production of Upsilon mesons in U+U collisions at 193 GeV at mid-rapidity (|y| < 1). Previous studies in central Au+Au collisions at 200 GeV show a suppression of Upsilon(1S+2S+3S) production relative to expectations from the Upsilon yield in p+p collisions scaled by the number of binary nucleon-nucleon collisions (Ncoll), with an indication that the Upsilon(1S) state is also suppressed. The present measurement extends the number of participant nucleons in the collision (Npart) by 20% compared to Au+Au collisions, and allows us to study a system with higher energy density. We observe a suppression in both the Upsilon(1S+2S+3S) and Upsilon(1S) yields in central U+U data, which consolidates and extends the previously observed suppression trend in Au+Au collisions.
Journal of the Physical Society of Japan | 1991
T. Kohno; K. Munakata; Takashi Imai; Akira Yoneda; C. Kato; Masaru Matsuoka; T. Doke; J. Kikuchi; Toshisuke Kashiwagi; K. Nishijima; Nobuyuki Hasebe; H. J. Crawford
A Heavy Ion cosmic ray Telescope (HIT) has been scheduled to be launched into the synchronous orbit in 1993 aiming to observe elemental and isotopic composition of solar energetic particles and galactic cosmic rays. In this paper, we report the results of accelerator beam experiments of a prototype model of HIT. The telescope consists of two dimensional Position Sensitive Detectors (PSDs) and energy loss detectors (PIN type and Li-drifted type). The mass resolution was 1.1 amu in FWHM for 110 MeV/n pure iron ( 56 Fe) beam. By exposing HIT to beams consisting of various nuclides produced by the projectile fragmentation process in a reaction induced by 56 Fe beam, we confirmed that the secondary elements from 16 S to 25 Mn were clearly separated and that also the isotopes were separated for each elements lighter than 22 Ti. The observed mass resolution was 0.57 amu, 0.66 amu and 0.82 amu in FWHM for 18 Ar, 20 Ca and 22 Ti, respectively. We can conclude that the HIT has good prospects of enough ability for o...
European Physical Journal C | 1982
T. F. Hoang; Bruce Cork; H. J. Crawford
AbstractResults of calculation of the fireball radius as measured by means of the Hanbury-Brown and Twiss (HBT) effect are interpreted in the context of Landaus hydrodynamical model. A method based on a simple geometric picture of fireball formation is used to deduce the pion radius. From available data of variousn
Physical Review C | 2016
L. Adamczyk; J. K. Adkins; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; I. Alekseev; A. Aparin; D. Arkhipkin; E. C. Aschenauer; A. Attri; G. S. Averichev; X. Bai; Bairathi; R. Bellwied; A. Bhasin; Ashok Kumar Bhati; P. Bhattarai; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; J. Bouchet; J. D. Brandenburg; A. V. Brandin; I. Bunzarov; J. M. Butterworth; H. Caines; M. Calderon De La Barca Sanchez; J. M. Campbell; D. Cebra