norma selomit ramírez uribe ific csic-uv....2021/06/15 · os. ramírez-uribe, a. e....
TRANSCRIPT
![Page 1: Norma Selomit Ramírez Uribe IFIC CSIC-UV....2021/06/15 · oS. Ramírez-Uribe, A. E. Rentería-Olivo, G. Rodrigo, G. F. R. Sborlini, and L. Vale Silva, “Quantum algorithm for Feynman](https://reader036.vdocuments.net/reader036/viewer/2022081622/613b3184f8f21c0c8268dcbe/html5/thumbnails/1.jpg)
Norma Selomit Ramírez UribeIFIC CSIC-UV.
PARTICLEFACE 2021: Working Group Meeting and Management Committee Meeting
July 15, 2021.
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Outline
q Motivation
q Loop-Tree Dualityq Brief historyq Notation
q 𝑁"MLT universal topology
q A look at quantum
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Motivation
Improve theoretical predictions
Achieve higher perturbative orders
Quantum fluctuations at high-energy scattering processes= Multiloop scattering amplitudes =
Loop diagrams
…
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Minkowski space Euclidean space
LTD-brief history
q What does LTD do?
Opens any loop diagram to a forest of non-disjoint trees.
q How does it do?
Exploits the Cauchy residue theorem to reduce the dimensionof the integration domain by one unit:
# #𝑑𝑞&
�
�
(𝐺*(𝑞,).
,/0𝒒= −2𝜋𝑖 # 7𝑅𝑒𝑠{<=?@A&}
�
𝒊
(𝐺*(𝑞,).
,/0?
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LTD-brief history
oBuchta, Chachamis, Draggiotis, Malamos and Rodrigo, JHEP 1411 (2014) 014
oHernández, Sborlini and Rodrigo, JHEP 1602 (2016) 044
oS. Buchta, G. Chachamis, P. Draggiotis and G. Rodrigo, EPJC 77 (2017) 274
Duality relation (LTD)
Singular behaviourat one-loop
FDU
Applications
oCatani, Gleisberg, Krauss, Rodrigo and Winter, JHEP 0809 (2008) 065
oBierenbaum, Catani, Draggiotis and Rodrigo, JHEP 1010 (2010) 073
oBierenbaum, Buchta, Draggiotis, Malamos and Rodrigo, JHEP 1303 (2013) 025
oDriencourt, Rodrigo and Sborlini, EPJC 78 (2018) no.3, 231
oDriencourt, Rodrigo, Sborlini and Torres, JHEP 1902 (2019) 143
oSborlini, Driencourt, Hernández and Rodrigo, JHEP 1608 (2016) 160
oSborlini, Driencourt and Rodrigo, JHEP 1610 (2016) 162
oAguilera, Driencourt, Plenter, Ramírez, Rodrigo, Sborlini, Torres and Tracz,JHEP 1912 (2019) 163
Causal and anomalous thresholds
oPlenter and Rodrigo, EPJC 81 (2021) 320 Asymptotic expansions
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LTD-brief historyoRunkel, Szor, Vesga and Weinzierl, Phys. Rev. Lett. 122 no.11, 111603 Erratum:
[Phys. Rev. Lett. 123 no.5, 059902]
oRunkel, Szor, Vesga and Weinzierl, Phys. Rev. D 101 (2020) 116014
oCapatti, Hirschi, Kermanschah and Ruijl, Phys. Rev. Lett. 123 (2019) no.15, 151602
oCapatti, Hirschi, Kermanschah, Pelloni and Ruijl, JHEP 04 (2020) 096
Alternative dual
representation
Reformulation of LTD to all orders
oAguilera, Driencourt, Hernández, Plenter, Ramírez, Rodrigo, Sborlini, Torres, Tracz, “Open loop amplitudes and causality to all orders and powers from the loop-tree duality”, Phys. Rev. Lett. 124 (2020) no.21, 211602
q Can we find explicit and more compact analytic expressions withthe LTD formalism to all orders?
Causality
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LTD-brief history𝑀𝐿𝑇 𝑁𝑀𝐿𝑇 𝑁G𝑀𝐿𝑇
oS. Ramırez-Uribe, R. J. Hernández-Pinto, G. Rodrigo, G. F. R. Sborlini, and W. J. Torres Bobadilla, “Universal opening of four-loop scattering amplitudes to trees,” JHEP 04, 129 (2021).
Multiloop topologies that first appear at four loops
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LTD-Notation
q A generic 𝐿-loop scattering amplitude with𝑁 external legs,
𝒜.I 1,… , 𝑛 = # 𝒜*
I 1,… , 𝑛ℓ𝟏,..,ℓ𝑳
#ℓR
= −𝑖𝜇"TU #𝑑Uℓ,2𝜋 U
�
�
𝒩 ℓ, I, 𝑝X .𝐺*(1,… , 𝑛)
( 𝐺* 𝑞,YR
�
,∈0∪⋯∪]
𝑞,G − 𝑚,G + 𝜄0 T0
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LTD-Notation
q The LTD representation is written in terms of nested residues,
𝒜bI 1,… , 𝑟; 𝑟 + 1,… , 𝐿 + 1 = −2𝜋𝑖 7 𝑅𝑒𝑠 𝒜b
I 1,… , 𝑟 − 1; 𝑟, … , 𝑛 , 𝐼𝑚𝜂 g 𝑞,h < 0�
𝒊𝒓∈𝒓On-shell Off-shell
starting from
𝒜bI 1; 2, … , 𝐿 + 1 = −2𝜋𝑖 7 𝑅𝑒𝑠 𝒜*
I 1,… , 𝐿 + 1 , 𝐼𝑚𝜂 g 𝑞,k < 0�
𝒊𝟏∈𝟏
𝜂l = 1, 𝟎
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𝑵𝟒𝑴𝑳𝑻 universal topology
12 3
4
5
12
23
123
234
L+ 1
1 2 3
4
5
12
123
34234
L+ 1
1 2 3
4
5
12
123
234
24
L+ 1
• 𝑞,r = ℓs + 𝑘,r, 𝑠 ∈ 1, … , 𝐿• 𝑞,(uvk) = −∑ ℓsI
s/0 + 𝑘, uvk• 𝑞,kx = −ℓ0 −ℓG +𝑘,kx• 𝑞,kxy = −ℓ0 −ℓG −ℓz + 𝑘,kxy• 𝑞,xy{ = −∑ ℓs"
s/G + 𝑘,xy{• 𝑞,hr = −ℓ| − ℓs + 𝑘,hr, 𝑟, 𝑠 ∈ 2, 3, 4
q Multiloop topologies that appear for the first time at four loops:
𝐽 ≡ 23 ∪ 34 ∪ 24
Can we achieve a unified description?
t-, s- and u- kinematic channels
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𝑵𝟒𝑴𝑳𝑻 universal topology
= 𝒜.{�I�" 1, 2, 3, 4, 12, 123, 234, 𝐽 ⊗𝒜�I�
IT" 5,… , 𝐿 + 1+𝒜.x�I�
z 1 ∪ 234, 2, 3, 4 ∪ 123, 12, 𝐽 ⊗𝒜�I�ITz 5�, … , 𝐿 + 1
Momentum flow reversed
J
1 2 3
4
5
12
123
234
L+ 1
=
J
1
12
2 3
123
234 4⊗
5
6
7
L+ 1
+
J
1
12
2 3 123
234 4
⊗
5
6
7
L+ 1
𝒜.{�I�I 1,… , 𝐿 + 1, 12, 123, 234, 𝐽
On-shell
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𝑵𝟒𝑴𝑳𝑻 universal topology
𝒜.{�I�" 1, 2, 3, 4, 12, 123, 234, 𝐽 = 𝒜.x�I�
" 1, 2, 3, 4, 12, 123, 234 ⊗𝒜 & 𝐽
+7𝒜b" 1, 2, 3, 4, 12, 123, 234, 𝒔
�
𝒔∈�
Off-shell
J
1
12
2 3
123
234 4
=
1
2
12
234
123
3
4+
1
12
2 3
23
123
234 4
+
1
12
2 3
123
234 4
34+
1
12
2 3
123
4 234
24
{𝟐𝟑, 𝟑𝟒, 𝟐𝟒}
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𝑵𝟒𝑴𝑳𝑻 universal topology
J
1
12
2 3123
234 4
=
1
12
2 3 123
234 4
+
1
12
2 3 123
234 4
23
+
1
12
2 3123
234 4
34
+
1
12
2
123 3
4
234
24
𝒜.x�I�z 1 ∪ 234, 2, 3, 4 ∪ 123, 12, 𝐽 = 𝒜.�I�
z 1 ∪ 234, 2, 3, 4 ∪ 123, 12 ⊗𝒜 & 𝐽
+7𝒜bz 1, 2, 3, 4, 12, 123, 234, 𝒔
�
𝒔∈�
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Causal representation
= # 𝒜.y�I�" (1, 2, 3, 4, 5, 12, 123, 234)
ℓ𝟏,..,ℓ𝑳
= #𝒩.y�I� 𝑞s,&
(�), 𝑘X,&
∏ 2𝑞s,&(�)I�"
s/0 ∏ 𝜆,�0z,/0 𝜆,Tℓk,..,ℓu
= # �𝒜.x�I�" 1, 2, 3, 4, 12, 123, 234
ℓk,..,ℓu
+ 𝒜.�I�z 1 ∪ 234, 2, 3, 4 ∪ 123, 12 ⊗𝒜b
0 5� �
Universal opening
Adding them all together
?
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Causal representation
1
2 3
4
5λ+1
1
12
3
4
234
λ+2
2
12
123
4
234
λ+3
2 3
123234
5λ+4
2 3
4234
λ+5
2 3
1231
λ+6
12 3
4
5λ+7
1 123
234 4
λ+8
122
234
5λ+9
1
2
12
λ+10
123
3
12
λ+11
123
4
5λ+12
1
234
5λ+13
= #1
𝑥𝑳�𝟒ℓk,..,ℓu
7𝒩𝝈(𝒊𝟏,…,𝒊𝟒) 𝑞s,&
(�), 𝑘X,&𝜆𝝈(𝒊𝟏)𝜆𝝈(𝒊𝟐)𝜆𝝈(𝒊𝟑)𝜆𝝈(𝒊𝟒)
�
�
Reinterpreting in terms of four entangled thresholds
( 2𝑞s,&(�)I�"
s/0
= LTD Causal representation =
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Causal representation
2 4 6 8 10
2
4
6
8
10
q12,0(+)
q 123,0
(+)
5.×10-6
0.000010
0.000015
0.000020
0.000025LTD representation
LTD causal representation
Clever analytical rearrangement
Impact of noncausal singularities
Integrand-level behaviour of the noncusal LTD representation of a four-loop 𝑁z𝑀𝐿𝑇 diagram.
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Causal representation
2
q12,0(+)
1.0620058x10-5
2
q12,0(+)
1.0620058x10-5
Numerical instabilities of the four-loop 𝑁z𝑀𝐿𝑇 intgrand arising due to noncausal singularities (left), which are absent in the causal representation (right).
Noncausal and causal evaluations of the 𝑁z𝑀𝐿𝑇 configurations.
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Causal representation
2 3
23
λ+14
4
23
234
λ+15
1 12323
λ+16
1
3
12
23
λ+17
1
45
23
λ+18
2
12
12323
λ+19
5
123
234
23
λ+20
2
4
5
12
23
λ+21
3
5
12
234
23
λ+22
1
24
4 3
123
λ(u)+16
1
24
5
12
123
λ+23
1
2
123
24
234
λ+24
𝒜.{�I�I 1, … , 𝐿 + 4, 𝐽 = #
1𝑥 �,s,� ,𝑳�𝟓
ℓk,..,ℓu
7𝒩𝝈(𝒊𝟏,…,𝒊𝟓) 𝑞s,&
(�), 𝑘X,&𝜆𝝈(𝒊𝟏)𝜆𝝈(𝒊𝟐)𝜆𝝈(𝒊𝟑)𝜆𝝈(𝒊𝟒)𝜆𝝈(𝒊𝟓)
�
�
2𝑞{Gz,z",G"},&(�) 𝑥I�"Extra causal configurations of the 𝑡 −channel
Extra causal configurations of the 𝑢 −channel
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A look at quantum
oS. Ramírez-Uribe, A. E. Rentería-Olivo, G. Rodrigo, G. F. R. Sborlini, and L. Vale Silva, “Quantum algorithm for Feynman loop integrals”, arXiv:2105.08703 [hep-ph]
Bootstrap the causal representation in the LTD of representative multiloop topologies.
0 1
2
0 1
2
34
0 1
2
3
4
5
0
1
2
3
4
56
7
0
1
2
3
4
5 6
7
8
0
1
2
3
4
5 6
7
8
0
1
2
3
4
5 6
7
8
Two possible states: |1⟩𝑜𝑟|0⟩
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A look at quantum1. Superposition 𝑁 = 2]
2. Oracle
3. Diffusion
Grover’s algorithm
|𝑞⟩ =1𝑁�7|𝑥⟩
|𝑞⟩ = cos 𝜃 |𝑞�⟩ + sin 𝜃 |𝑤⟩o Superposition
Orthogonal state
Winning state
Mixing angle
𝜃|𝑞�⟩
|𝑤⟩|𝒒⟩
|𝑤⟩ =1𝑟�7|𝑥⟩�
¢∈£
|𝑞�⟩ =1𝑁 − 𝑟� 7|𝑥⟩
�
¢∈£
θ = arcsin 𝑟/𝑁�
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A look at quantum
o Oracle 𝑈£ = 𝑰 − 2|𝑤⟩⟨𝑤| 𝑈£|𝑥⟩ = «−|𝑥⟩ 𝑖𝑓𝑥 ∈ 𝑤
|𝑥⟩ 𝑖𝑓𝑥 ∉ 𝑤
𝜃|𝑞�⟩
|𝑤⟩
2𝜃
−|𝑤⟩𝑼𝒘|𝒙⟩
Flips the state |𝑞⟩ if 𝑞 ∈ 𝑤 and leaves it unchanged otherwise.
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A look at quantum
o Diffusion 𝑈? = 2|𝑞⟩⟨𝑞| − 𝑰
𝜃|𝑞�⟩
|𝑤⟩
2𝜃
−|𝑤⟩
4𝜃
𝑈?𝑈£|𝑞⟩
Performs a reflection around theinitial state |𝑞⟩
The iterative application of the oracle and diffusion operators t times leads to:
𝑈?𝑈£�|𝑞⟩ = cos 𝜃� |𝑞�⟩ + sin 𝜃� |𝑤⟩
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A look at quantum
4𝜃
𝜃|𝑞�⟩
|𝑤⟩
2𝜃
−|𝑤⟩
𝑈?𝑈£|𝑞⟩
To consider: 𝜃 ≤ 𝜋/6 𝑟/𝑁 ≤ 1/4 ?
78/256 204/512 230/512204/512
39/256 102/512 102/512 115/512
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A look at quantum
|𝑞⟩
|𝑐⟩
|𝑎⟩
o Oracle
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A look at quantum|00000111〉 |00101101〉 |01111011〉 |11110101〉
|000001011〉 |100111001〉 |111000111〉 |001111001〉
|000101101〉 |010100111〉 |110111101〉 |111100011〉
|000101001〉 |100001101〉 |000100101〉 |111000111〉
𝟑𝟗/𝟐𝟓𝟔
𝟏𝟎𝟐/𝟓𝟏𝟐
𝟏𝟎𝟐/𝟓𝟏𝟐
Requires 33 qubits > Qiskit capacity
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Conclusions
q We have obtained a very compact dual representation for selected looptopologies to all orders up to four loops, which exhibits a nested form interms of simpler topologies. We conjecture that this factorization works atall orders.
q The 𝑁"𝑀𝐿𝑇 universal topology allow us to describe any scatteringamplitude up to four-loop.
q The causal LTD representation is interpreted in terms of entangledcausal thresholds and allows a more efficient numerical evaluation ofmultiloop scattering amplitudes.
q Causal configurations of multiloop Feynman integrals have beenidentified with the application of Grover’s quantum algorithm.
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