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Separating fact from fantasy*: The chiral anomaly and the proton spin puzzle Raju Venugopalan (BNL) Arizona State Online Theory Colloquium, August 19, 2020 Separating fact from fantasy*: The chiral anomaly and the proton spin puzzle R. L.


  1. Separating fact from fantasy*: The chiral anomaly and the proton spin puzzle Raju Venugopalan (BNL) Arizona State Online Theory Colloquium, August 19, 2020

  2. Separating fact from fantasy*: The chiral anomaly and the proton spin puzzle R. L. Jaffe A. Manohar 30th anniversary of their seminal paper which strongly inspired the work reported here: The G(1) Problem: Fact and Fantasy on the Spin of the Proton. Nucl. Phys., B337:509–546, 1990

  3. Work* in collaboration with Andrey Tarasov (The OSU and CFNS) * Our first paper will be on arXiv tonight (6 pm ASU time) and two others are in preparation

  4. Talk outline v Polarized DIS – preliminaries v Iso-singlet axial vector current and topology of QCD vacuum: the role of the triangle graph v Fun with world-lines v World-line effective action: i) Finding a triangle in a box in Bjorken and Regge asymptotics ii) Hidden triangles dress infrared poles; the WZW term iii) Small x Bj effective action for polarized DIS: Extended PCAC and the 𝜃 ′ as an emergent axion-like field iv) QCD evolution of the small x effective action v Conjecture: How spin diffuses from polarized large x partons to small x via sphalerons transitions v General considerations/outlook

  5. On the DOE web page: January 9, 2020 WASHINGTON, D.C. – Today, the U.S. Department of Energy (DOE) announced the selection of Brookhaven National Laboratory in Upton, NY, as the site for a planned major new nuclear physics research facility. The Electron Ion Collider (EIC), to be designed and constructed over ten years at an estimated cost between $1.6 and $2.6 billion, will smash electrons into protons and heavier atomic nuclei in an effort to penetrate the mysteries of the “strong force” that binds the atomic nucleus together. “The EIC promises to keep America in the forefront of nuclear physics research and particle accelerator technology, critical components of overall U.S. leadership in science,” said U.S. Secretary of Energy Dan Brouillette . “This facility will deepen our understanding of nature and is expected to be the source of insights ultimately leading to new technology and innovation.” “ Secretary Brouillette also approved Critical Decision-0, “Approve Mission Need,” for the EIC on December 19, 2019

  6. What’s the Electron-Ion Collider ?

  7. The deeply inelastic scattering (DIS) femtoscope 2 2 2 Measure of Q q ( k k ) ' = − = − − µ µ resolution power & ' θ # 2 2 e Q 4 E E sin ' = $ ! e e 2 % " pq E ' & ' θ # Measure of inelasticity 2 e e y 1 cos = = − $ ! pk E 2 % " e 2 2 Q Q Bjorken variable: Measure of x = = momentum fraction of struck 2 pq sy quark Inclusive DIS measurements: e+ ↑ p/A à e’+X Measure only the scattered lepton in the detector: structure functions (pdfs: F2,FL,g1,g2,…) Semi-inclusive DIS (SIDIS) measurements : e+ ↑ p/A à e’+h(p,K,p,jet)+X Measure electrons in coincidence with identified hadrons/jets (Transverse momentum dependent dists. -TMDs) Exclusive measurements (DVCS,…): e+ ↑ p/A à e’+ photon/hadron + p/A Measure electron, photon (or e.g., vector meson), intact proton/nucleus (Generalized parton dists. -GPDs) Diffractive measurements : e+ ↑ p/A à e’+ hadrons/jets + rapidity gap (coherent diff. → 𝐣𝐨𝐮𝐛𝐝𝐮 𝐪/𝐁) As for exclusive, but with rapidity veto on particle production (Diff. structure functions, F 2D , F LD ) Also, measure nuclear fragments, multiparticle correlations, …

  8. Landscape of scattering in the strong interaction Aschenauer et al., arXiv:1708.01527 Rep.Prog. Phys. 82, 024301 (2019) Higher twists Many open questions: three-D structure, spin and orbital dynamics, many-body correlations, small x

  9. The Electron-Ion Collider Polarized protons up to 275 GeV; Nuclei up to ~ Z/A*275 GeV/n Ø Existing RHIC complex: Storage (Yellow), injectors (source, booster, AGS) Ø Need few modifications Ø RHIC beam parameters fairly close to those required for EIC@BNL Electrons up to 18 GeV Ø Storage ring, provides the range sqrt(s) = 20-140 GeV. Beam current limited by RF power of 10 MW Ø Electron beam with variable spin pattern (s) accelerated in on- energy, spin transparent injector (Rapid-Cycling-Synchrotron) with 1-2 Hz cycle frequency Ø Polarized e-source and a 400 MeV s-band injector LINAC in v Electron storage ring with frequent injection of the existing tunnel fresh polarized electron bunches v Hadron storage ring with strong cooling or Design optimized to reach 10 34 cm -2 sec -1 frequent injection of hadron bunches

  10. The Electron-Ion Collider Ø First polarized electron-polarized proton collider Ø First electron-nucleus collider Ø Luminosities up to ~ 1000 times that of HERA Ø Fine resolution inside the proton down to ~10 -18 m

  11. A long and winding road… 1 st eRHIC workshop, Symbol is born! (BNL Arts departmen BNL Dec. 3-4, 1999 2012 EIC white paper 2018 BNL 1212.1701.v3 (Garvey,Ludlam,McLerran, A. Accardi et al Strikman,Venugopalan) Report NAS panel � 2010 INT report Redux: 2018 2018 Week 4: History of EIC Project 1999/2000 2007 LRP 2015 2002 LRP �

  12. Polarized DIS at small x – reaching into terra incognita with EIC

  13. The proton’s spin puzzle: a many-body picture Fixed target DIS experiments showed that quarks ( ΔΣ ) carry only about 30% of the proton’s spin “Spin crisis”: failure of the quark model (“Ellis-Jaffe sum rule”) picture of relativistic “constituent” quarks Evidence for gluon spin ( ∆𝐻) from RHIC but large uncertainties from small x D. De Florian, R. Sassot, M. Stratmann, W. Vogelsang, PRL 113 (2014)

  14. <latexit sha1_base64="tQOc+mW+4IKZvfVKiUAPE5LepX0=">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</latexit> <latexit sha1_base64="tQOc+mW+4IKZvfVKiUAPE5LepX0=">ACT3icbVFNaxsxFNQ6bZO4H3HaYy6ipuCMbsh0B5D0OCa2TgOUsb2XtWlgfG+ltGrP4H+aS3vo3eumhJVR29B8DAiGmRHvaZSVSnqM4x9Ra+3J02frG5vt5y9evtrqbL8+8bZyXAy5VdadZeCFkYMUaISZ6UToDMlTrPZwdI/vRTOS2u+4rwUYw2FkbnkgEFKOzn7LBQCZV9koYH2js931NWOluipUwaTOPzhE6uKOsXadK76q8ClDlZTBGcs9+CU7MspzVzml5U4Gasz/qUW4NOZtVyzGKRdrxIF6BPiRJQ7qkwVHa+c4mldaGOQKvB8lcYnjGhxKrsSizSovSuAzKMQoUANa+HG96mNB3wVlQnPrwjFIV+r/N2rQ3s91FpIacOrve0vxMW9UYf5xXEtTVigM/zcorxQNXS3LpRPpBEc1DwS4k2FXyqfgGP4gnYoIbn/5IfkZHeQxIPkeK+7/6mpY4PskLekRxLygeyTQ3JEhoSTa/KT/CZ/opvoV3TbaqKtqCFvyB20Nv8COxtA=</latexit> <latexit sha1_base64="tQOc+mW+4IKZvfVKiUAPE5LepX0=">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</latexit> <latexit sha1_base64="tQOc+mW+4IKZvfVKiUAPE5LepX0=">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</latexit> Resolving the proton’s spin puzzle: the g 1 structure function 50 g 1 extracted g 1 (x,Q 2 ) + const(x) x=5.2 × 10 -5 (+53) - from longitudinal spin asymmetry DSSV 2014 8.2 × 10 -5 (+45) 90% C.L. ∆ g 40 EIC 15 × 100 GeV 1.3 × 10 -4 (+38) EIC 15 × 250 GeV Z 1 EIC 20 × 250 GeV ∆Σ ( Q 2 ) ∝ dx g 1 ( x, Q 2 ) → quark contribution 2.1 × 10 -4 (+33) 30 0 3.3 × 10 -4 (+28) 5.2 × 10 -4 (+24) 8.2 × 10 -4 (+21) dramatic reduction 1.3 × 10 -3 (+19) 20 ? dg 1 2.1 × 10 -3 (+17) of uncertainties: ~ −Δ g ( x , Q 2 ) → gluon contr. 3.3 × 10 -3 (+15.5) d log( Q 2 ) 5.2 × 10 -3 (+14) 8.2 × 10 -3 (+13) 1.3 × 10 -2 (+12) 2.1 × 10 -2 (+11) 3.3 × 10 -2 (+10) 10 5.2 × 10 -2 (+9) 8.2 × 10 -2 (+8) w o r l d now d a t a 1.3 × 10 -1 (+7) 2.1 × 10 -1 (+6) u n t i l e R eRHIC H 3.3 × 10 -1 (+5) I C 5.2 × 10 -1 (+4) 10 2 10 3 1 10 Q 2 [GeV 2 ]

  15. Resolving the proton’s spin puzzle: the g 1 structure function Aschenauer et al., arXiv:1708.01527 Rep. Prog. Phys. 82, 024301 (2019)

  16. Iso-singlet axial vector current and topology of the QCD vacuum Reviews: S. D. Bass, RMP, hep-ph/0411005 G. M. Shore, hep-ph/0701171

  17. g 1 structure function: formal definitions Hadron tensor 𝑋 "# = with 𝑋 "# is the antisymmetric part of 𝑋 "# where 2 Most generally, 𝑇 " = $% & ! 𝑄 " and 𝜇 = ±1/2 Generalized parton model (“leading twist”): Where the quark helicity pdf is defined to be

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