Christopher Monroe
Quantum Computing
with Atoms
Computing and Information
Alan Turing (1912-1954)
universal computing machines
Claude Shannon (1916-2001)
quantify information: the bit
𝐻 = −
𝑖=1
𝑘
𝑝
𝑖
𝑙𝑜𝑔
2
𝑝
𝑖
moving CPU memory tape read/write device 0110
1 1 0 0
1
1
ENIAC (1946)
МЭСМ (1949)
Colossus (1943)
vacuum
tubes
solid-state
transistor
(1947)
Moore’s Law
exponential growth in computing
Transistor density relative to 1978
1980 1990 2000 2010 2018 100,000 10,000 1,000 100 10 1
There's Plenty of Room at the Bottom
(1959)
“
When we get to the very, very small world
–
say circuits of
seven atoms
–
we have a lot of new things that would happen
that represent
completely new opportunities for design
. Atoms
on a small scale behave like nothing on a large scale, for they
satisfy the
laws of quantum mechanics…”
Richard
Feynman
Quantum bits
entanglement: “wiring
without wires
”
superposition
a
|0
+
b|1
|0
state
|1
state
Quantum Information Science
|0
state
Prob = |
a
|
2|1
state
Prob = |
b
|
2measurement:
“state collapse”
Entanglement
superposition
a
|0
|0
+
b|1|1
|0
|0
state
|1|1
state
OR
Good News…
parallel processing
on
2
Ninputs
a
0|000
+
a
1|001
+
a
2|010
+
a
3|011
a
4|100
+
a
5|101
+
a
6|110
+
a
7|111
f(x)
N=300 qubits have more
configurations than there are
particles in the universe!
e.g., N=3
qubits
…Bad News…
measurement gives
random result
f(x)
depends
on
all
inputs
…Good News!
quantum interference
David Deutsch
(early 1990s)
A quantum computer can factor numbers
exponentially faster
than classical computers
39 = 3
13
(…easy)
38647884621009387621432325631 =
?
?
P. Shor (1994)
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39quantum
wavefunction
𝜓(𝑛)
Application: Optimization
Traveling Salesman problem
what is the
shortest path
through N
cities?
Molecular Simulations
•
designer materials
•
new catalysts
•
protein folding
A quantum computer differs more from a laptop…
Quantum Computer Technologies
adapted from
Science, Dec 2016
IonQ, Honeywell Intel, HRL, SQC Microsoft
Neutral atoms
Neutral atoms, like ions, store qubits within electronic states. Interactions through excitation to Rydberg states 1 97% 20
Many qubits, 2D and maybe 3D
Lasers needed, spaghetti physics, atoms escape
Technologies QuEra ColdQuanta
Photonics
Photonic qubits interact via linear elements
Linear optical gates, integrated on-chip No memory, not clear how to scale
Xanadu
Google, Quantum Diamond Atom Computing PsiQuantum
2
S
1/2
|
=
|0,0
|
=
|1,0
Atomic (hyperfine) qubit (
171
Yb
+
)
n
HF/2
p
=
12.642 812 118 GHz
2
S
1/2
2
P
1/2
369 nm
2.1 GHzg/2p
= 20 MHz
|
|
# photons collected in 50 ms Probabilit y 0 10 20 30 40 50 60|
171
Yb
+
Qubit Detection
n
HF/2
p
=
12.642 812 118 GHz
2
S
1/2
2
P
1/2
369 nm
g/2p
= 20 MHz
|
|
2.1 GHz # photons collected in 50 ms Probabilit y 0 10 20 30 40 50 60|
171
Yb
+
Qubit Detection
High-NA collection + SNSPD (J. Kim, Duke)
- 6.5% of fluorescence detected
-
99.93% qubit detection in 12
m
s
171
Yb
+
Qubit Manipulation
D
= 33 THz
355 nm
2
P
3/2
g/2p
= 20 MHz
n
HF=
12.642 812 118 GHz
|
(100 MHz, 10psec)
D. Hayes et al., PRL 104, 140501 (2010)
66 THz
2
P
1/2
2
S
1/2
|
𝑔
1𝑔
2Monroe Group
Atomic Physics Lab
Photo: Phil Schewe
ENIAC (1946)
МЭСМ (1949)
Colossus (1943)
Quantum Computer Optical Controller
Laser
………..
32-channel
AOM
power stabilizer rep rate stabilizer beam-pointing stabilizer beam-pointing stabilizerDOE
rf inputs (200MHz)AOM
S. Debnath,...
Nature
536
, 63 (2016)
N. Linke,...
PNAS
114
, 13 (2017)
Full “Quantum Stack” architecture
Quantum Computer Optical Controller
Laser
………..
32-channel
AOM
power stabilizer rep rate stabilizer beam-pointing stabilizer beam-pointing stabilizerDOE
rf inputs (200MHz)AOM
S. Debnath,...
Nature
536
, 63 (2016)
N. Linke,...
PNAS
114
, 13 (2017)
Year Application
Reference
Collaborator
Institute
2013 Frustration and AFM order Science 340, 583 J. Freericks Georgetown 2014 Lieb-Robinson propagation Nature 511, 198 A. Gorshkov NIST
2015 Spin-1 Dynamics Phys. Rev. X 5, 021026 A. Retzker Hebrew University 2016 Manybody Localization Nat. Physics 12, 907 D. Huse, P. Hauke Princeton, Innsbruck 2017 Hidden Shift, Toffoli-3 Gate PNAS 114, 13 M. Roetteler Microsoft, Inc.
Grover Nat. Comm. 8, 1918 D. Maslov NSF Toffoli-4 Gate Thesis, Debnath D. Maslov NSF Prethermalization Science Adv. 3, e1700672 Z. Gong, A. Gorshkov NIST Time Crystaline Order Nature 543, 217 N. Yao Berkeley Dynamical Phase Transition Nature 551, 601 A. Gorshkov NIST [[4,2,2]] Error Detection Science Adv. 3, e1701074 K. Brown Duke 2018 Fredkin Gate, Fermi-Hubbard PRA 98, 052334 S. Johri Intel Corp.
Bayesian Game QST 3, 045002 N. Solmeyer ARL Qubit Detection ML J. Phys. B 51 174006 M. Hafezi JQI 2019 Full Adder, Parallel CNOTs Nature 567, 61 D. Maslov NSF
Generative Modeling ML Science Adv. 5, eaaw9918 A. Perdomo-Ortiz NASA
Deuteron VQE Simulation PRA 100, 62319 R. Pooser, O. Shehab ORNL, IonQ Validating stabilizer states Phys. Rev. A 99, 042337 Amir Kalev QuICS UMD
Quantum Scrambling Nature 567, 61 B. Yoshida, N. Yao Perimeter, Berkeley Circuit QAOA arXiv:1906.02699 T. Hsieh, S. Johri Perimeter, Intel Corp. Benchmarks and Comparison arXiv: 1905.11349 M. Martonosi Princeton
Analog QAOA arXiv:1906.02700 A. Gorshkov, S. Jordan NIST, Microsoft Inc. Quasiparticle Confinement arXiv: 1912.11117 A. Gorshkov NIST
Efficient QAOA (Max-Cut, Deuteron) arXiv:1906.00476 Isaac Kim, Omar Shehab Stanford, IonQ Dynamical mean field theory arxiv: 1910.04735 Ross Duncan, Ivan Rungger Cambridge QC, NPL
Year Application
Reference
Collaborator
Institute
2020 Many-body dephasing arXiv: 2001.02477 F. Marquardt MPL Erlangen Quantum walks theory arXiv:2001.11197 B. Radhakrishnan, C. Chandrashekar ARL, Chennai Quantum walks, cellular automaton arXiv:2002.02537 B. Radhakrishnan, C. Chandrashekar ARL, Chennai [[9,1,3]] Bacon/Shor code arXiv:2009.11482 K. Brown Duke
NMR Deconvolution in progress E. Demler Harvard
Measurement-induced phase xsition in progress M. Gullens, D. Huse, N. Yao NIST, Princeton, Berkeley Classical Verification of QC in progress U. Vazarani, N. Yao, T. Vidick Berkeley, CalTech
Cross platform benchmarking in progress Peter Zoller Innsbruck Lattice Gauge Thy in progress Z. Davoudi UMD Ising Scattering in progress Yannick Meurice U. Iowa Circuit-based MBL in progress Sonika Johri Intel Corp. Schwinger model simulation in progress Zohreh Davoudi UMD
Envariance measures in progress Wojciech Zurek Los Alamos Para-particle simulations in progress C. M. Alderete, Blas R. Lara UMD, INAOE Edge-cover problem QAOA in progress B. Sundar, K. Hazzard Innsbruck, Rice Lee-Yang Zeroes in progress Lex Kemper NCSU
Triangle game in progress Akimasa Miyake UNM Molecular Cluster simulations in progress Nicolas Sawaya Intel Corp. Ring-molecule dynamics Q-Sim in progress Rob Parrish QCWare Chaos-QAOA in progress Gregory Quiroz, O. Shehab APL, IonQ GAN-compression of circuits in progress Xiaodi Wu QuICS UMD QFT- based benchmarking in progress Yannick Meurice U. Iowa Block-diagonalization via Grover in progress Sonika Johri Intel Corp. term-ordered VQE in progress M. Martonosi Princeton Cluster state generation in progress Robert Raussendorf, Vito Scarola UBC, VaTech Block-optimized VQE in progress Peter Zoller Innsbruck
Norbert Linke
(UMD/JQI)
Marko Cetina
(UMD/JQI)
new faculty @Duke
Crystal Noel
(UMD/JQI)
new faculty @Duke
(1) Prepare spins along
𝑥
(2) Quench spins to
(3) Measure along
𝑥
increase
𝑩/𝑱
𝐻 =
𝑖<𝑗𝑱
|𝑖 − 𝑗|
𝛼𝜎
𝑥𝑖𝜎
𝑥 𝑗+ 𝑩
𝑖𝜎
𝑧𝑖order
along
𝑥
align
along
𝑧
A. Gorshkov (JQI/NIST)
D. Huse (Princeton)
S. Johri (Intel)
N=53
qubits
𝐵/𝐽
20
18
16
14
12
0 0.5 1.0 1.5 2.0
avg
. l
arges
t domain
size
Exotic Magnetism
Cosmology + Quantum Gravity
Quantum Scrambling
Scrambling
: “complete diffusion” of quantum information, relevant to information evolution in black holes
N. Yao (UC Berkeley)
B. Yoshida (Perimeter)
L. Susskind (Stanford)
EPR
EPR
EPR
EPR
ۧ
|0
ۧ
|𝜓
ۧ
|0
ۧ
|0
ۧ
|0
ۧ
|0
ۧ
|0
ۧ
|𝜓
𝑈
𝑈
†
Bell
Bell
Bell
†
input
qubit
Successful teleportation if U
scrambles
output
qubit
Landsman, et al., Nature 567, 61 (2019)
In 1935, Einstein and Rosen showed that
widely-separated black holes can be connected by a tunnel
through space-time, now known as a
wormhole
Physicists suspect that the connection in a wormhole
and the connection in quantum entanglement
are the same thing, just on a vastly different scale!
entanglementNature 417, 709 (2002)
Science Advances 3, e1601540 (2017)
Shuttling between
multiple zones
Linear shuttling through
single zone
>100 qubits
Quantum Computer Scaling I
NIST-Boulder
Univ. Mainz
Technology:
Integrated photonics and
switches, SNSPD detector array
Plan:
Multicore quantum
processing
optical switch detector array QMem QCommSingle trapped 138Ba+atom beam-splitter optical fiber
photo-detector photo-detector
ns pulses @ 100 kHz
p ~ 4%
Making single photons
S
1/2P
1/2D
3/2649.7nm
mJ=+3/2 mJ=-1/2 mJ=+1/2138
Ba
+
493.4nm
t
=10ns
mJ=+1/2t
(
m
s)
t
(
m
s)
𝑔
2(𝜏)
𝑔
2(𝜏)
coincidence count rate
𝑔
2(0)
Higginbottom, et al. (Innsbruck), New J. Phys. 18, 093038 (2016)
Single trapped 174Yb+atom beam-splitter optical fiber
photo-detector photo-detector
2ps pulses @ 5.3 MHz
l
=369nm
g (2 ) (t)excellent single photon source
Making single photons
p
~ 3%
delay (ns)
𝑔
2(0)
Higginbottom, et al. (Innsbruck), New J. Phys. 18, 093038 (2016)
C. Crocker, et al., Optics Express 27, 28143 (2019)
-1000 -500 0 500 1000
P. Maunz, et al., Nature Physics 3, 538 (2007)
Single trapped 174Yb+atom beam-splitter optical fibers
photo-detector photo-detector
delay (ns)
Hong, Ou, Mandel, PRL 59, 2044 (1987) Y.H. Shih & C. O. Alley, PRL 61, 2921 (1988)
Santori, et al., Nature, 419, 594 (2002) Kaltenbaek, et al, PRL, 96, 240502 (2006) Legero, et al., PRL, 93, 070503 (2004). Thompson, et al., Science, 313, 74 (2006). Felinto, et al. Nature Physics, 2, 844 (2006). Beugnon, et al. Nature, 440, 779 (2006). P. Maunz, et al., Nature Physics 3, 538 (2007)
g(2)(t) 2ps pulses @ 8.1 MHz Single trapped 174Yb+atom
T
integ~ minutes
p
2~
10
-31 meter
2-photon interference
spinless atom
(no qubit)
Heralded coincident events:
(H
1& V
2) or (V
1& H
2)
→ |
↓↑
-
|
↓↑
(H
1& V
1) or (V
2& H
2)
→ |
↓↑
+
|
↓↑
(H
1& H
1) or (H
2& H
2)
→ |
↓↓
(V
1& V
1) or (V
2& V
2)
→ |
↑↑
Photonic Linkage between Atomic Qubits
𝑅
𝑒𝑛𝑡=
1
2
𝑅𝑝
2
D. Hucul, et al., Nature Phys. 11, 37 (2015)
C. Balance, et al, Phys. Rev. Lett. 124, 110501
Current State-of-art:
𝑝 = 𝜂
𝐷𝑇
𝑑Ω
4𝜋
= .35 .6 .1 = 2%
𝑅 = 1 𝑀𝐻𝑧
𝑹
𝒆𝒏𝒕
≈ 𝟏𝟖𝟎 𝒔𝒆𝒄
−𝟏
Hong, Ou, Mandel, PRL 59, 2044 (1987) Y.H. Shih & C. O. Alley, PRL 61, 2921 (1988) Simon & Irvine, PRL 91, 110405 (2003) L.-M. Duan, et. al., QIC 4, 165 (2004) Y. L. Lim, et al., PRL 95, 030505 (2005)
2007: Trapped Ions[Nature 449, 68–71] 2013: Trapped Neutrals[PRL 110, 140403] 2014: NV-diamond[Science 345, 532] 2015: Quantum Dots[Nature Phys. 12, 218] 2016: Superconductors[PRX 6, 031036] Single trapped 171Yb+atom beam-splitter optical fibers
photo-detector photo-detector
2ps pulses @ 8.1 MHz Single trapped 171Yb+ atom
p
2~
10
-31 meter
Duan and Monroe, Rev. Mod. Phys. 82, 1209 (2010) Li and Benjamin, New J. Phys. 14, 093008 (2012) Monroe, et al., Phys. Rev. A 89, 022317 (2014)