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Quantum Technology:
Chris
Monroe
University of Maryland
Department of Physics
National Institute of
Standards and Technology
Putting Weirdness to Use
atom-sized
transistors
2040
molecular-sized
transistors
2025
Quantum mechanics
and computing
“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…”
“There's Plenty of Room
at the Bottom” (1959)
Richard Feynman
Quantum
Mechanics
Information
Theory
Quantum Information Science
A new science for the 21st Century?
20th Century
21st Century
Computer Science and Information Theory
i
k
i
i ppH 2
1
log

Alan Turing (1912-1954)
universal computing machines
Claude Shannon (1916-2001)
quantify information: the bit
Charles Babbage (1791-1871)
mechanical difference engine
ENIAC
(1946)
The first solid-state transistor
(Bardeen, Brattain & Shockley, 1947)
Albert Einstein (1879-1955)
Erwin Schrödinger (1887-1961)
Werner Heisenberg (1901-1976)
Quantum Mechanics: A 20th century revolution in physics
• Why doesn’t the electron collapse onto the nucleus of an atom?
• Why are there thermodynamic anomalies in materials at low temperature?
• Why is light emitted at discrete colors?
• . . . .
The Golden Rules
of Quantum Mechanics
Rule #2: Rule #1 holds as long as you don’t look!
|0 and |1
Rule #1: Quantum objects are waves and can
be in states of superposition.
“qubit”: |0 and |1
|1|0
or
probability p 1-p
GOOD NEWS…
quantum parallel processing on 2N inputs
Example: N=3 qubits
 = a0 |000 + a1|001 + a2 |010 + a3 |011
a4 |100 + a5|101 + a6 |110 + a7 |111 f(x)
…BAD NEWS…
Measurement gives random result
e.g.,   |101
f(x)
N=300 qubits: more information
than particles in the universe!
depends on
all inputs
…GOOD NEWS!
quantum interference
|0  |0 + |1
|1  |1  |0
quantum
NOT gate:
e.g., |0 + |1 |0  |0|0 + |1|1
superposition  entanglement
( )
…GOOD NEWS!
quantum interference
depends on
all inputs
quantum
logic gates
|0 |0  |0 |0
|0 |1  |0 |1
|1 |0  |1 |1
|1 |1  |1 |0
quantum
XOR gate:
Quantum State: [0][0] & [1][1]
John Bell (1964)
Any possible “completion” to
quantum mechanics will
violate local realism
just the same
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
1 1
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
0 0
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
0 0
1 1
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
0 0
1 1
1 1
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
0 0
1 1
1 1
1 1
Entanglement: Quantum Coins
Two coins in a
quantum
superposition
[H][H] & [T][T]
0 0
1 1
0 0
1 1
1 1
1 1
0 0
. .
. .
. .
Application: quantum cryptographic key distribution
+
plaintext
KEY
ciphertext
ciphertext
KEY
plaintext
+
Quantum Superposition
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Superposition
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Superposition
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Entanglement
“Spooky action-at-a-distance”
(A. Einstein)
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Entanglement
“Spooky action-at-a-distance”
(A. Einstein)
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Entanglement
“Spooky action-at-a-distance”
(A. Einstein)
From Taking the Quantum Leap, by Fred Alan Wolf
Quantum Entanglement
“Spooky action-at-a-distance”
(A. Einstein)
From Taking the Quantum Leap, by Fred Alan Wolf
David Deutsch
“When a quantum
measurement is made,
the universe bifucates!”
• Many Universes
• Multiverse
• Many Worlds
David Deutsch (1985)
Peter Shor (1994)
Lov Grover (1996)
fast number factoring N = pq
fast database search
Quantum
Computers
and Computing
Institute of
Computer Science
Russian Academy
of Science
ISSN 1607-9817
0
500
1000
1500
2000
2500
3000
# articles mentioning “Quantum Information”
or “Quantum Computing”
Nature
Science
Phys. Rev. Lett.
Phys. Rev.
2005200019951990 2010
Quantum Factoring
A quantum computer can factor numbers
exponentially faster than classical computers
15 = 3  5
38647884621009387621432325631 = ?  ?
Look for a joint property of all 2N inputs
e.g.: the periodicity of a function
P. Shor, SIAM J. Comput. 26, 1474 (1997)
A. Ekert and R. Jozsa, Rev. Mod. Phys. 68, 733 (1996)
application: cryptanalysis (N ~ 10200)
𝑓 𝑥 = sin 2𝜋
𝑥
𝑝
p = period
𝑓𝑎 𝑥 = 𝑎 𝑥(𝑀𝑜𝑑 𝑁) r = period (a = parameter)
x 2x 2x (Mod 15)
0 1 1
1 2 2
2 4 4
3 8 8
4 16 1
5 32 2
6 64 4
7 128 8
8 256 1
etc…
Error-correction Shannon (1948)
Redundant encoding to protect against (rare) errors
better off whenever p < 1/2
𝑝 → 3𝑝2
1 − 𝑝 + 𝑝3
0/1
potential error: bit flip
p(error) = p
0/1
1/0
𝑝(𝑒𝑟𝑟𝑜𝑟) = 3𝑝2 1 − 𝑝 + 𝑝3
000/111
000/111
potential error: bit flip
010/101 etc..
take majority
Decoherence
|0 + |1
P0 C
C* P1
r 
|0 + |1  /4{ |00000 + |10010 + |01001 + |10100
+ |01010  |11011  |00110  |11000
 |11101  |00011  |11110  |01111
 |10001  |01100  |10111 + |00101 }
+ /4{ |11111 + |01101 + |10110 + |01011
+ |10101  |00100  |11001  |00111
 |00010  |11100  |00001  |10000
 |01110  |10011  |01000 + |11010 }
5-qubit code
corrects all
1-qubit errors
to first order
Quantum error-correction Shor (1995)
Steane (1996)
Trapped Atomic Ions
Yb+ crystal
~5 mm
C.M. & D. J. Wineland, Sci. Am., 64 (Aug 2008)
R. Blatt & D. J. Wineland, Nature 453, 1008 (2008)
State |
N
S
N
S
Quantum bit inside an atom:
States of relative electron/nuclear spin
State |
S
N
N
S
“Perfect” quantum measurement of a single atom
state | state |
# photons collected in 200ms
Probability
3020100
0
0.2
atom fluoresces 108 photons/sec
laser laser
atom remains dark
3020100
0
1
# photons collected in 200ms
>99% detection efficiency!
Cirac and Zoller, Phys. Rev. Lett. 74, 4091 (1995)
Trapped Ion Quantum Computer
Internal states of these ions entangled
AFM ground state order 222 events
Antiferromagnetic Néel order of N=10 spins
441 events out of 2600 = 17%
Prob of any state at random =2 x (1/210) = 0.2%
219 events
All in state 
All in state 
2600 runs, =1.12
a (C.O.M.)
b (stretch)
c (Egyptian)
d (stretch-2)
Mode competition –
example: axial modes, N = 4 ions
Fluorescencecounts
Raman Detuning dR (MHz)
-15 -10 -5 0 5 10 15
20
40
60
a
b
c
d
a
b
c
d
2a
c-a
b-a
2b,a+c
b+c
a+b
2a
c-a
b-a
2b,a+c
b+c
a+b
carrier
axial modes only
mode
amplitudes
(see K. Brown)
1 mm
GaTech
Res. Inst.
Al/Si/SiO2
Maryland/LPS
GaAs/AlGaAs
Sandia Nat’l Lab: Si/SiO2
NIST-Boulder
Au/Quartz
optical fiber
trapped
ions
trapped
ions
Photonic Quantum Networking
Linking ideal quantum memory (trapped ion) with ideal
quantum communication channel (photon)
unknown qubit
uploaded to
atom #1
| + |
qubit transfered to
atom #2
| & |
Quantum teleportation
of a single atom
S. Olmschenk et al., Science 323, 486 (2009).
we need
more time..
and more
qubits..
Large scale vision (103 – 106 atomic qubits)
• 1 layer of transistors, 9-12 layers of connectors
• Interconnect complexity determines circuit complexity
• Efficient transport of bits in the computer is crucial
ibm.com
Classical Computer Architecture
Physics
Chemistry
Computer Science
Electrical Engineering
Mathematics
Information Theory
Quantum
Mechanics
Information
Theory
Quantum Information Science
A new science for the 21st Century?
20th Century
21st Century
Quantum Computing Abyss
?
noise
reduction
new
technology
error
correction
efficient
algorithms
 20 >1000
<100 >109
theoretical requirements
for “useful” QC
state-of-the-art
experiments
# quantum bits
# logic gates
Quantum Information Hardware at
Other condensed-matter
single atomic impurities in glass
single phosphorus atoms in silicon
Semiconductors
quantum dots
2D electron gases
Superconductors
Cooper-pair boxes (charge qubits)
rf-SQUIDS (flux qubits)
Individual atoms and photons
ion traps
atoms in optical lattices
cavity-QED
ENIAC
(1946)
1947
We have always had a great deal of difficulty in understanding
the world view that quantum mechanics represents…
…Okay, I still get nervous with it…
It has not yet become obvious to me that there is no real
problem. I cannot define the real problem, therefore I suspect
there’s no real problem, but I’m not sure there’s no real problem.
Richard Feynman (1982)
N=1028
N=1
Postdocs
Susan Clark (Sandia)
Wes Campbell (UCLA)
Taeyoung Choi
Chenglin Cao
Brian Neyenhuis
Phil Richerme
Grahame Vittorini
Collaborators
Luming Duan
Howard Carmichael
Jim Freericks
Alexey Gorshkov
Grad Students
David Campos
Clay Crocker
Shantanu Debnath
Caroline Figgatt
Dave Hayes (Sydney)
David Hucul
Volkan Inlek
Rajibul Islam (Harvard)
Aaron Lee
Kale Johnson
Simcha Korenblit
Andrew Manning
Jonathan Mizrahi
Crystal Senko
Jake Smith
Ken Wright
Undergrads
Daniel Brennan
Geoffrey Ji
Katie Hergenreder
ARO
JOINT
QUANTUM
INSTITUTE
www.iontrap.umd.edu
NSA

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Quantum technology

  • 1. Quantum Technology: Chris Monroe University of Maryland Department of Physics National Institute of Standards and Technology Putting Weirdness to Use
  • 3. “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…” “There's Plenty of Room at the Bottom” (1959) Richard Feynman
  • 4. Quantum Mechanics Information Theory Quantum Information Science A new science for the 21st Century? 20th Century 21st Century
  • 5. Computer Science and Information Theory i k i i ppH 2 1 log  Alan Turing (1912-1954) universal computing machines Claude Shannon (1916-2001) quantify information: the bit Charles Babbage (1791-1871) mechanical difference engine
  • 7. The first solid-state transistor (Bardeen, Brattain & Shockley, 1947)
  • 8. Albert Einstein (1879-1955) Erwin Schrödinger (1887-1961) Werner Heisenberg (1901-1976) Quantum Mechanics: A 20th century revolution in physics • Why doesn’t the electron collapse onto the nucleus of an atom? • Why are there thermodynamic anomalies in materials at low temperature? • Why is light emitted at discrete colors? • . . . .
  • 9. The Golden Rules of Quantum Mechanics Rule #2: Rule #1 holds as long as you don’t look! |0 and |1 Rule #1: Quantum objects are waves and can be in states of superposition. “qubit”: |0 and |1 |1|0 or probability p 1-p
  • 10. GOOD NEWS… quantum parallel processing on 2N inputs Example: N=3 qubits  = a0 |000 + a1|001 + a2 |010 + a3 |011 a4 |100 + a5|101 + a6 |110 + a7 |111 f(x) …BAD NEWS… Measurement gives random result e.g.,   |101 f(x) N=300 qubits: more information than particles in the universe!
  • 11. depends on all inputs …GOOD NEWS! quantum interference
  • 12. |0  |0 + |1 |1  |1  |0 quantum NOT gate: e.g., |0 + |1 |0  |0|0 + |1|1 superposition  entanglement ( ) …GOOD NEWS! quantum interference depends on all inputs quantum logic gates |0 |0  |0 |0 |0 |1  |0 |1 |1 |0  |1 |1 |1 |1  |1 |0 quantum XOR gate:
  • 13. Quantum State: [0][0] & [1][1] John Bell (1964) Any possible “completion” to quantum mechanics will violate local realism just the same
  • 14. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 1 1
  • 15. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1
  • 16. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1 0 0
  • 17. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1 0 0 1 1
  • 18. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1 0 0 1 1 1 1
  • 19. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1 0 0 1 1 1 1 1 1
  • 20. Entanglement: Quantum Coins Two coins in a quantum superposition [H][H] & [T][T] 0 0 1 1 0 0 1 1 1 1 1 1 0 0 . . . . . .
  • 21. Application: quantum cryptographic key distribution + plaintext KEY ciphertext ciphertext KEY plaintext +
  • 22. Quantum Superposition From Taking the Quantum Leap, by Fred Alan Wolf
  • 23. Quantum Superposition From Taking the Quantum Leap, by Fred Alan Wolf
  • 24. Quantum Superposition From Taking the Quantum Leap, by Fred Alan Wolf
  • 25. Quantum Entanglement “Spooky action-at-a-distance” (A. Einstein) From Taking the Quantum Leap, by Fred Alan Wolf
  • 26. Quantum Entanglement “Spooky action-at-a-distance” (A. Einstein) From Taking the Quantum Leap, by Fred Alan Wolf
  • 27. Quantum Entanglement “Spooky action-at-a-distance” (A. Einstein) From Taking the Quantum Leap, by Fred Alan Wolf
  • 28. Quantum Entanglement “Spooky action-at-a-distance” (A. Einstein) From Taking the Quantum Leap, by Fred Alan Wolf
  • 29. David Deutsch “When a quantum measurement is made, the universe bifucates!” • Many Universes • Multiverse • Many Worlds
  • 30.
  • 31. David Deutsch (1985) Peter Shor (1994) Lov Grover (1996) fast number factoring N = pq fast database search Quantum Computers and Computing Institute of Computer Science Russian Academy of Science ISSN 1607-9817 0 500 1000 1500 2000 2500 3000 # articles mentioning “Quantum Information” or “Quantum Computing” Nature Science Phys. Rev. Lett. Phys. Rev. 2005200019951990 2010
  • 32. Quantum Factoring A quantum computer can factor numbers exponentially faster than classical computers 15 = 3  5 38647884621009387621432325631 = ?  ? Look for a joint property of all 2N inputs e.g.: the periodicity of a function P. Shor, SIAM J. Comput. 26, 1474 (1997) A. Ekert and R. Jozsa, Rev. Mod. Phys. 68, 733 (1996) application: cryptanalysis (N ~ 10200) 𝑓 𝑥 = sin 2𝜋 𝑥 𝑝 p = period 𝑓𝑎 𝑥 = 𝑎 𝑥(𝑀𝑜𝑑 𝑁) r = period (a = parameter) x 2x 2x (Mod 15) 0 1 1 1 2 2 2 4 4 3 8 8 4 16 1 5 32 2 6 64 4 7 128 8 8 256 1 etc…
  • 33. Error-correction Shannon (1948) Redundant encoding to protect against (rare) errors better off whenever p < 1/2 𝑝 → 3𝑝2 1 − 𝑝 + 𝑝3 0/1 potential error: bit flip p(error) = p 0/1 1/0 𝑝(𝑒𝑟𝑟𝑜𝑟) = 3𝑝2 1 − 𝑝 + 𝑝3 000/111 000/111 potential error: bit flip 010/101 etc.. take majority
  • 34. Decoherence |0 + |1 P0 C C* P1 r  |0 + |1  /4{ |00000 + |10010 + |01001 + |10100 + |01010  |11011  |00110  |11000  |11101  |00011  |11110  |01111  |10001  |01100  |10111 + |00101 } + /4{ |11111 + |01101 + |10110 + |01011 + |10101  |00100  |11001  |00111  |00010  |11100  |00001  |10000  |01110  |10011  |01000 + |11010 } 5-qubit code corrects all 1-qubit errors to first order Quantum error-correction Shor (1995) Steane (1996)
  • 35.
  • 36. Trapped Atomic Ions Yb+ crystal ~5 mm C.M. & D. J. Wineland, Sci. Am., 64 (Aug 2008) R. Blatt & D. J. Wineland, Nature 453, 1008 (2008)
  • 37. State | N S N S Quantum bit inside an atom: States of relative electron/nuclear spin State | S N N S
  • 38.
  • 39. “Perfect” quantum measurement of a single atom state | state | # photons collected in 200ms Probability 3020100 0 0.2 atom fluoresces 108 photons/sec laser laser atom remains dark 3020100 0 1 # photons collected in 200ms >99% detection efficiency!
  • 40. Cirac and Zoller, Phys. Rev. Lett. 74, 4091 (1995) Trapped Ion Quantum Computer Internal states of these ions entangled
  • 41.
  • 42. AFM ground state order 222 events Antiferromagnetic Néel order of N=10 spins 441 events out of 2600 = 17% Prob of any state at random =2 x (1/210) = 0.2% 219 events All in state  All in state  2600 runs, =1.12
  • 43. a (C.O.M.) b (stretch) c (Egyptian) d (stretch-2) Mode competition – example: axial modes, N = 4 ions Fluorescencecounts Raman Detuning dR (MHz) -15 -10 -5 0 5 10 15 20 40 60 a b c d a b c d 2a c-a b-a 2b,a+c b+c a+b 2a c-a b-a 2b,a+c b+c a+b carrier axial modes only mode amplitudes (see K. Brown)
  • 44. 1 mm
  • 46. optical fiber trapped ions trapped ions Photonic Quantum Networking Linking ideal quantum memory (trapped ion) with ideal quantum communication channel (photon)
  • 47.
  • 48. unknown qubit uploaded to atom #1 | + | qubit transfered to atom #2 | & | Quantum teleportation of a single atom S. Olmschenk et al., Science 323, 486 (2009).
  • 49. we need more time.. and more qubits..
  • 50. Large scale vision (103 – 106 atomic qubits)
  • 51. • 1 layer of transistors, 9-12 layers of connectors • Interconnect complexity determines circuit complexity • Efficient transport of bits in the computer is crucial ibm.com Classical Computer Architecture
  • 52.
  • 53. Physics Chemistry Computer Science Electrical Engineering Mathematics Information Theory Quantum Mechanics Information Theory Quantum Information Science A new science for the 21st Century? 20th Century 21st Century
  • 54. Quantum Computing Abyss ? noise reduction new technology error correction efficient algorithms  20 >1000 <100 >109 theoretical requirements for “useful” QC state-of-the-art experiments # quantum bits # logic gates
  • 55.
  • 56. Quantum Information Hardware at Other condensed-matter single atomic impurities in glass single phosphorus atoms in silicon Semiconductors quantum dots 2D electron gases Superconductors Cooper-pair boxes (charge qubits) rf-SQUIDS (flux qubits) Individual atoms and photons ion traps atoms in optical lattices cavity-QED
  • 57.
  • 59.
  • 60. We have always had a great deal of difficulty in understanding the world view that quantum mechanics represents… …Okay, I still get nervous with it… It has not yet become obvious to me that there is no real problem. I cannot define the real problem, therefore I suspect there’s no real problem, but I’m not sure there’s no real problem. Richard Feynman (1982)
  • 62. Postdocs Susan Clark (Sandia) Wes Campbell (UCLA) Taeyoung Choi Chenglin Cao Brian Neyenhuis Phil Richerme Grahame Vittorini Collaborators Luming Duan Howard Carmichael Jim Freericks Alexey Gorshkov Grad Students David Campos Clay Crocker Shantanu Debnath Caroline Figgatt Dave Hayes (Sydney) David Hucul Volkan Inlek Rajibul Islam (Harvard) Aaron Lee Kale Johnson Simcha Korenblit Andrew Manning Jonathan Mizrahi Crystal Senko Jake Smith Ken Wright Undergrads Daniel Brennan Geoffrey Ji Katie Hergenreder ARO JOINT QUANTUM INSTITUTE www.iontrap.umd.edu NSA