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Pion Valence Quark Distribution from Lattice Calculable Current-Current Correlations Colin Egerer In Collaboration with R. Sufian, J. Karpie, K. Orginos, J. Qiu & D. Richards

Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

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Page 1: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Pion Valence Quark Distribution from Lattice Calculable Current-Current Correlations

Colin EgererIn Collaboration with R. Sufian, J. Karpie, K. Orginos, J. Qiu & D. Richards

Page 2: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

➔ Models not a complete picture

➔ Global analysis techniques not uniquely defined

➔ Not fully known

An Essential Window into Hadronic Structure

2

➔ Essential for interpretation of high-energy scattering data & BSM searches at energy frontier

DIS

Parton Model

PDFs - non-perturbative

pQCD

M. Tanabashi et al. (Particle Data Group), Phys. Rev. D 98, 030001 (2018)

Page 3: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Outline

3

➔ An essential window

➔ Lattice QCD and Light-Cone Physics?

➔ Lattice “Cross Sections”

➔ The pion - an economical theater

➔ Numerical Investigation

◆ Ensemble specifics

◆ Pion valence distribution

◆ Results and comparison with literature

➔ Progress & Outlook

Page 4: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

A Non-perturbative Study of QCD

4

➔ Low-energies & a strong coupling

➔ Real time path integral

Page 5: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

A Non-perturbative Study of QCD

4

➔ Low-energies & a strong coupling

➔ Real time path integral

Uncountably infinite parameter space

➔ Lattice QCD discretize and Wick rotate to imaginary time

➔ Importance sampling

Tremendous success in studying QCD spectrum and accessing state-to-vacuum transitions

Page 6: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Towards the Extraction of PDFs from the Lattice

5

➔ All light-cone physics is lost in a Euclidean spacetime

➔ Moments calculations & the OPE

◆ Power-divergent mixing/gauge noise for high moments

➔ Led to quasi/pseudo-PDF proposals

X. Ji, Phys. Rev. Lett. 110, 262002 (2013), arXiv:1305.1539 [hep-ph]

K. Orginos, A. Radyushkin, J. Karpie, and S. Zafeiropoulos, Phys. Rev. D96, 094503 (2017), arXiv:1706.05373 [hep-ph]

?!

Page 7: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Towards the Extraction of PDFs from the Lattice

5

➔ All light-cone physics is lost in a Euclidean spacetime

➔ Moments calculations & the OPE

◆ Power-divergent mixing/gauge noise for high moments

➔ Led to quasi/pseudo-PDF proposals

X. Ji, Phys. Rev. Lett. 110, 262002 (2013), arXiv:1305.1539 [hep-ph]

K. Orginos, A. Radyushkin, J. Karpie, and S. Zafeiropoulos, Phys. Rev. D96, 094503 (2017), arXiv:1706.05373 [hep-ph]

?!

➢ Beyond quasi-/pseudo-PDF approaches

○ Hadronic Tensor (K. F. Liu et al., Phys. Rev. Lett. 72, Phys. Rev. D 59 & D 62)○ Auxiliary quark methods (U. Aglietti et al., Phys. Lett. B441; W. Detmold & C.J. D. Lin, Phys. Rev.

D73; V. Braun & D. Mueller, Eur. Phys. J. C55)○ “OPE without OPE” (A. J. Chambers et al., Phys. Rev. Lett. 118)

Page 8: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Lattice “Cross Sections” (LCS)

6

Y. Q. Ma & J. W. Qiu, Phys. Rev. D 98, no. 7, 074021 (2018), arXiv:1404.6860 [hep-ph]Y. Q. Ma & J. W. Qiu, Phys. Rev. Lett. 120, no. 2, 022003 (2018), arXiv:1709.03018 [hep-ph]

➢ Defining properties:

○ calculable in LQCD with Euclidean time

○ well-defined continuum limit; UV finite

○ share same collinear div. w/ PDFs

➢ Single-hadron matrix elements of renormalized non-local ops.

PDFsPseudo-structure Functions

Hard Coefficients

valid for any finite provided

Page 9: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Pion Structure - A First Numerical LCS Study

7

➔ Chiefly from pionic Drell-Yan

➔ Importance of pion cannot be understated

◆ DCSB and long-range interaction◆ nucleon quark sea flavor asymmetry

E.g. J. S. Conway et al., Phys. Rev. D 39, 39 (1989)J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985)

Page 10: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

PR12-15-006: TDIS @ JLab(pion structure via Sullivan process)

Pion Structure - A First Numerical LCS Study

7

➔ Chiefly from pionic Drell-Yan

➔ Importance of pion cannot be understated

◆ DCSB and long-range interaction◆ nucleon quark sea flavor asymmetry

J. S. Conway et al., Phys. Rev. D 39, 39 (1989)

E.g. J. S. Conway et al., Phys. Rev. D 39, 39 (1989)J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985)

LO Analysis Conflicts with Expectations

Page 11: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

PR12-15-006: TDIS @ JLab(pion structure via Sullivan process)

Pion Structure - A First Numerical LCS Study

7

➔ Chiefly from pionic Drell-Yan

➔ Importance of pion cannot be understated

◆ DCSB and long-range interaction◆ nucleon quark sea flavor asymmetry

Can a LCS calculation serve as a discriminator?

J. S. Conway et al., Phys. Rev. D 39, 39 (1989)

E.g. J. S. Conway et al., Phys. Rev. D 39, 39 (1989)J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985)

LO Analysis Conflicts with Expectations

Page 12: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Many Wick Contractions

8

➔ 4pt function with light-quark currents

Page 13: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Many Wick Contractions

8

➔ 4pt function with light-quark currents

Page 14: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Many Wick Contractions

8

➔ Heavy-light currents

◆ sufficiently small and leading-twist contribution to PDFW. Detmold & C.J. D. Lin, Phys.Rev. D73 (2006) 014501 hep-lat/0507007

Page 15: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Currents to Consider

9

➔ Vector/axial currents pseudo-scalar hadrons

Page 16: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Currents to Consider

9

➔ Vector/axial currents pseudo-scalar hadrons

➔ Isolation of pseudo-structure functions

Page 17: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Currents to Consider

9

➔ Vector/axial currents pseudo-scalar hadrons

➔ Isolation of pseudo-structure functions

➔ Selecting: and

Page 18: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Matching Kernels

10

➔ Factorized relation asymptotic parton state order-by-order in

Page 19: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Matching Kernels

10

➔ Factorized relation asymptotic parton state order-by-order in

Page 20: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Matching Kernels

10

➔ Factorized relation asymptotic parton state order-by-order in

Page 21: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Essence of the Calculation

11

➔ Randomly chosen source point

➔ Momentum projections and src/snk seps.

◆ ...costly inversions

➢ Unrestricted energy flow

➢ Heavy auxiliary quark propagators

W. Detmold & C.J. D. Lin, Phys.Rev. D73 (2006) 014501 hep-lat/0507007

High-momenta essential

Page 22: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Essence of the Calculation

11

➔ Randomly chosen source point

➔ Momentum projections and src/snk seps.

◆ ...costly inversions

➢ Unrestricted energy flow

➢ Heavy auxiliary quark propagators

W. Detmold & C.J. D. Lin, Phys.Rev. D73 (2006) 014501 hep-lat/0507007

High-momenta essential

Page 23: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Essence of the Calculation

11

➔ Randomly chosen source point

➔ Momentum projections and src/snk seps.

◆ ...costly inversions

➢ Unrestricted energy flow

➢ Heavy auxiliary quark propagators

W. Detmold & C.J. D. Lin, Phys.Rev. D73 (2006) 014501 hep-lat/0507007

High-momenta essential

Page 24: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Essence of the Calculation

11

➔ Randomly chosen source point

➔ Momentum projections and src/snk seps.

◆ ...costly inversions

➢ Unrestricted energy flow

➢ Heavy auxiliary quark propagators

W. Detmold & C.J. D. Lin, Phys.Rev. D73 (2006) 014501 hep-lat/0507007

High-momenta essential

Page 25: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Ensemble & Typical Ratio Fits

12

Page 26: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Pseudo-structure Function

13

➢ An ill-posed inverse !

➔ How best to extract PDFs?

➢ Extra information needed

Page 27: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

The Pseudo-structure Function

13

➢ An ill-posed inverse !

➔ Smooth, physically-motivated models

➔ ROOT for numerical integration Rene Brun & Fons Rademakers, Nucl. Inst. & Meth. in Phys. Res. A 389 (1997) 81-86

➔ How best to extract PDFs?

➢ Extra information needed

Page 28: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Extracted Valence PDF

14

Page 29: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Comparison with the Literature

15

R. Sufian, J. Karpie, CE et al., (2019) arXiv:1901.03921 [hep-lat]**To appear in PRD**

➔ Appear to be capturing essential physics --- gluons esp. important in pion

P. C. Barry et al., Phys. Rev. Lett. 121, 152001 (2018), arXiv:1804.01965 [hep-ph]

➔ commensurate

➔ consistent w/ NLL threshold soft-gluon resummation effects (ASV)

➔ favors

➔ no statistically meaningful change in distribution as varied

Page 30: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

In Progress

16

➔ Populating with off-axis separations

◆ maintaining

◆ improving statistics

Discretization effects...

Momentum projections as a time-slice average

G. S. Bali et al., Phys. Rev. D 98, no. 9, 094507 (2018), arXiv:1807.06671 [hep-lat]G. S. Bali et al., Eur. Phys. J. C78 (2018) no. 3, 217, arXiv:1709.04325 [hep-lat]

Page 31: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

In Progress

16

➔ Populating with off-axis separations

◆ maintaining

◆ improving statistics

➔ Completing isolation of NLO kernels

◆ logarithmic corrections ( and related )

◆ power corrections & higher-twist effects

Discretization effects...

Momentum projections as a time-slice average

G. S. Bali et al., Phys. Rev. D 98, no. 9, 094507 (2018), arXiv:1807.06671 [hep-lat]G. S. Bali et al., Eur. Phys. J. C78 (2018) no. 3, 217, arXiv:1709.04325 [hep-lat]

Page 32: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

In Progress

16

➔ Populating with off-axis separations

◆ maintaining

◆ improving statistics

➔ Completing isolation of NLO kernels

◆ logarithmic corrections ( and related )

◆ power corrections & higher-twist effects

➔ Finite volume effects?

➔ Power of LCS formalism lies in a “global” analysis of calculated matrix elements◆ analyzing

◆ Can LCS data be competitive enough to include in global analyses?

Discretization effects...

Momentum projections as a time-slice average

R. Briceño et al., Phys. Rev. D 98, no. 1, 014511 (2018), arXiv:1805.01034 [hep-lat]

G. S. Bali et al., Phys. Rev. D 98, no. 9, 094507 (2018), arXiv:1807.06671 [hep-lat]G. S. Bali et al., Eur. Phys. J. C78 (2018) no. 3, 217, arXiv:1709.04325 [hep-lat]

Page 33: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

BACKUPS

Page 34: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

More on quasi/pseudo-distributions

18

X. Ji, Phys. Rev. Lett. 110, 262002 (2013), arXiv:1305.1539 [hep-ph]

K. Orginos, A. Radyushkin, J. Karpie, and S. Zafeiropoulos, Phys. Rev. D96, 094503 (2017), arXiv:1706.05373 [hep-ph]

Fourier transform over length of Wilson line

Fourier transform Ioffe time - fixed length Wilson line

K. Cichy & M. Constantinou, arXiv:1811.07248v1 [hep-lat]

Page 35: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Leading Order Coefficient Functions - Coordinate Space

19

Page 36: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Matching Kernels & the Pion Valence Distribution

10

➔ Factorized relation asymptotic parton state order-by-order in

➔ To ensure access to valence distribution◆ momentum space pseudo-structure fns.

Y. Q. Ma & J. W. Qiu, Phys. Rev. Lett. 120, no. 2, 022003 (2018), arXiv:1709.03018 [hep-ph]

Page 37: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

➔ Solution of QCD from first-principles

➔ “No free lunch!”

◆ signal-to-noise problems

◆ excited-state contamination

◆ reduced symmetry groups

◆ discretization/finite volume effects

◆ quark mass dependence

➔ Systematics can be systematically removed with further computation...

Physics in a Discretized Euclidean Box

20

Page 38: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Momentum Smearing

21

➔ Dilemma >>>>>>> Large Ioffe time large momentum

G. S. Bali et al. Phys. Rev. D93, 094515 (2016), arXiv:1602.05525 [hep-lat]➔ Rotate gauge links

*** But what are these phases? ***

Page 39: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Scanning for Momentum Phases

22

Page 40: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

Preliminary E2 Pseudo-structure Functions

23

Many Combinations….

Vector-Vector of E1 ensemble

Page 41: Pion Valence Quark Distribution from Lattice Calculable ...J. Badier et all., Z. Phys. C18, 281 (1983) B. Betev et al., Z. Phys. C28, 9 (1985) LO Analysis Conflicts with Expectations

➔ Correlation fns. carry spacetime signature info

◆ time-indep matrix elements do not

➔ quasi-PDF carries no info about spacetime signature

➔ spacetime signature of ops. only arise when time-evolved

◆ should carry no E vs. M distinction

Euclidean vs. Minkowski Matrix Elements

24

➔ With no temporal extent

◆ 1-loop perturbative calculation (scalar field theory)

◆ all-orders derivation of LSZ reduction in Euclidean space

R. A. Briceño et al., Phys. Rev. D 96, no. 1, 014502 (2017), arXiv:1703.06072