L. C. Bland
Brookhaven National Laboratory
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Featured researches published by L. C. Bland.
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.
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 A | 2017
E. C. Aschenauer; Ian Balitsky; L. C. Bland; Stanley J. Brodsky; Matthias Burkardt; Volker D. Burkert; Jian Ping Chen; A. Deshpande; Markus Diehl; Leonard Gamberg; Matthias Grosse Perdekamp; Jin Huang; C. E. Hyde; Xiangdong Ji; Xiaodong Jiang; Zhong-Bo Kang; V. Kubarovsky; J. G. Lajoie; Keh-Fei Liu; Ming Liu; Simonetta Liuti; Wally Melnitchouk; P.J. Mulders; Alexei Prokudin; Andrey Tarasov; Jian Wei Qiu; Anatoly Radyushkin; David G. Richards; Ernst Sichtermann; Marco Stratmann
Abstract.A polarized ep/eA collider (Electron-Ion Collider, or EIC), with polarized proton and light-ion beams and unpolarized heavy-ion beams with a variable center-of-mass energy
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
sqrt{s} sim 20
Archive | 2011
E. C. Aschenauer; L. C. Bland; H. Crawford; Y. Goto; O. Eyser; Zhong-Bo Kang; A. Vossen
s∼20 to
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
sim 100
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
E. G. Judd; L. C. Bland; H. J. Crawford; J. Engelage; J. M. Landgraf; W. J. Llope; J. M. Nelson; M. Ng; A. Ogawa; C. Perkins; G. Visser; Z. J. Xu
∼100 GeV (upgradable to
Physical Review Letters | 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; Aditi Banerjee; 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; John M. Campbell
sim 150
Physical Review Letters | 2012
L. Adamczyk; G. Agakishiev; M. M. Aggarwal; Z. Ahammed; A Alakhverdyants; I. Alekseev; J Alford; B. D. Anderson; C D Anson; D. Arkhipkin; G. S. Averichev; J. Balewski; Aditi Banerjee; Z Barnovska; D R Beavis; R. Bellwied; M J Betancourt; R R Betts; A. Bhasin; Ashok Kumar Bhati; H. Bichsel; Jaroslav Bielcik; J. Bielcikova; L. C. Bland; I. Bordyuzhin; W Borowski; J. Bouchet; A. V. Brandin; S G Brovko; E Bruna
∼150 GeV) and a luminosity up to