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PSPACE. PostBQP. BQP. NP. P. Computational Intractability As A Law of Physics. Scott Aaronson University of Waterloo. GOLDBACH CONJECTURE: TRUE NEXT QUESTION. Things we never see…. YES. YES. Warp drive. Ü bercomputer. Perpetuum mobile.

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computational intractability as a law of physics

PSPACE

PostBQP

BQP

NP

P

Computational Intractability As A Law of Physics

Scott Aaronson

University of Waterloo

things we never see

GOLDBACH CONJECTURE: TRUE

NEXT QUESTION

Things we never see…

YES

YES

Warp drive

Übercomputer

Perpetuum mobile

Is the absence of these devices something physicists should think about?

Goal of talk: Convince you to see the impossibility of übercomputers as a basic principle of physics

computer science 101
Computer Science 101

Problem: “Given a graph, is it connected?”

Each particular graph is an instance

The size of the instance, n, is the number of bits needed to specify it

An algorithm is polynomial-time if it uses at most knc steps, for some constants k,c

P is the class of all problems that have polynomial-time algorithms

np nondeterministic polynomial time
NP: Nondeterministic Polynomial Time

Does

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have a prime factor ending in 7?

np hard if you can solve it you can solve everything in np
NP-hard: If you can solve it, you can solve everything in NP

NP-complete: NP-hard and in NP

Is there a Hamilton cycle (tour that visits each vertex exactly once)?

slide7

Hamilton cycleSteiner treeGraph 3-coloringSatisfiabilityMaximum clique…

Matrix permanentHalting problem…

FactoringGraph isomorphism…

Graph connectivityPrimality testingMatrix determinantLinear programming…

NP-hard

NP-complete

NP

P

does p np
Does P=NP?

No.

The (literally) $1,000,000 question

Q: What if P=NP, and the algorithm takes n10000 steps?

A: Then we’d just change the question!

Q: Why is it so hard to prove PNP?

A: Mostly because algorithms can be so clever!

what about quantum computers
What about quantum computers?

BQP: Bounded-Error Quantum Polynomial-Time

Shor 1994:BQP contains integer factoring

But factoring isn’t believed to be NP-complete.So the question remains: can quantum computers solve NP-complete problems efficiently?

Bennett et al. 1997: “Quantum magic” won’t be enough

If we throw away the problem structure, and just consider a “landscape” of 2n possible solutions, even a quantum computer needs ~2n/2 steps to find a correct solution

quantum adiabatic algorithm farhi et al 2000
Quantum Adiabatic Algorithm (Farhi et al. 2000)

Hi

Hf

Hamiltonian with easily-prepared ground state

Ground state encodes solution to NP-complete problem

Problem: Eigenvalue gap can be exponentially small

other alleged ways to solve np complete problems
Other Alleged Ways to Solve NP-complete Problems

Dip two glass plates with pegs between them into soapy water; let the soap bubbles form a minimum “Steiner tree” connecting the pegs (thereby solving a known NP-complete problem)

Protein folding: Can also get stuck at local optima (e.g., Mad Cow Disease)

DNA computers: Just massively parallel classical computers!

what would the world actually be like if we could solve np complete problems efficiently

Proof of Riemann hypothesis with 10,000,000 symbols?

Shortest efficient description of stock market data?

If there actually were a machine with [running time] ~Kn (or even only with ~Kn2), this would have consequences of the greatest magnitude.—Gödel to von Neumann, 1956

What would the world actually be like if we could solve NP-complete problems efficiently?
slide13

The NP Hardness AssumptionThere is no physical means to solve NP complete problems in polynomial time.

Rest of talk: Show how complexity yields a new perspective on linearity of QM, anthropic postselection, closed timelike curves, and initial conditions

Alright, what can we say about this assumption?

  • Implies, but is stronger than, PNP
  • As falsifiable as it gets
  • Consistent with currently-known physical theory
  • Scientifically fruitful?
1 nonlinear variants of the schr dinger equation

Can take as an additional argument for why QM is linear

1. Nonlinear variants of the Schrödinger Equation

Abrams & Lloyd 1998: If quantum mechanics were nonlinear, one could exploit that to solve NP-complete problems in polynomial time

1 solution to NP-complete problem

No solutions

2 anthropic principle
2. Anthropic Principle

Foolproof way to solve NP-complete problems in polynomial time (at least in the Many-Worlds Interpretation):

First guess a random solution. Then, if it’s wrong, kill yourself!

NP Hardness Assumption yields a nontrivial constraint on anthropic theorizing: no use of the Anthropic Principle can be valid, if its validity would give us a way to solve NP-complete problems in polynomial time

Technicality: If there are no solutions, you’re out of luck!

Solution: With tiny probability don’t do anything. Then, if you find yourself in a universe where you didn’t do anything, there probably were no solutions, since otherwise you would’ve found one!

what if we combine quantum computing with the anthropic principle
What if we combine quantum computing with the Anthropic Principle?

I.e. perform a polynomial-time quantum computation, but where we can measure a qubit and assume the outcome will be |1

Leads to a new complexity class: PostBQP(Postselected BQP)

Certainly PostBQP contains NP—but is it even bigger than that?

slide17

Some more animals from the complexity zoo…

PSPACE: Class of problems solvable with a polynomial amount of memory

PP: Class of problems of the form, “out of 2n possible solutions, are at least half of them correct?”

Adleman, DeMarrais, Huang 1998: BQPPP

Proof: Feynman path integral

Proof easily extends to show PostBQPPP

slide18

PSPACE

PP

PostBQP

NP

BQP

P

  • 2004:PostBQP=PP

In other words, quantum postselection gives exactly the power of PP

Surprising part:

This characterization yields a half-page proof of a celebrated result of Beigel, Reingold, and Spielman, that PP is closed under intersection

3 time travel

3. Time Travel

Everyone’s first idea for a time travel computer: Do an arbitrarily long computation, then send the answer back in time to before you started

THIS DOES NOT WORK

  • Why not?
  • Ignores the Grandfather Paradox
  • Doesn’t take into account the computation you’ll have to do after getting the answer
slide20

Deutsch’s Model

A closed timelike curve (CTC) is a computational resource that, given an efficiently computable function f:{0,1}n{0,1}n, immediately finds a fixed point of f—that is, an x such that f(x)=x

Admittedly, not every f has a fixed point

But there’s always a distribution D such that f(D)=D

Probabilistic Resolution of the Grandfather Paradox- You’re born with ½ probability- If you’re born, you back and kill your grandfather- Hence you’re born with ½ probability

slide21

Let PCTC be the class of problems solvable in polynomial time, if for any function f:{0,1}n{0,1}n described by a poly-size circuit, we can immediately get an x{0,1}n such that f(m)(x)=x for some m

Theorem:PCTC = PSPACE

Proof: PCTCPSPACE is easy

For PSPACEPCTC: Let sinit, sacc, and srej be the initial, accepting, and rejecting states of a PSPACE machine, and let (s) be the successor state of s. Then set

The only fixed point is an infinite loop, with b set to its “true” value

slide22

What if we perform a quantum computation around a CTC?

Let BQPCTC be the class of problems solvable in quantum polynomial time, if for any superoperator E described by a quantum circuit, we can immediately get a mixed state  such that E() = 

Clearly PSPACE=PCTCBQPCTC

A., Watrous 2006:BQPCTC = PSPACE

If closed timelike curves exist, then quantum computers are no more powerful than classical ones

slide23

Let vec() be a “vectorization” of . We can reduce the problem to the following: given a 22n22n matrix M, prepare a state  such that

Solution: Let

Then by Taylor expansion,

BQPCTCPSPACE: Proof Sketch

Hence P projects onto the fixed points of M

Furthermore, we can compute P exactly in PSPACE, using Csanky’s parallel algorithm for matrix inversion

4 initial conditions

|

4. Initial Conditions

Normally we assume a quantum computer starts in an “all-0” state, |0…0. But what if much better initial states were created in the Big Bang, and have been sitting around ever since?

Leads to the concept of quantum advice…

Useful?

slide25

Let BQP/qpoly be the class of problems solvable in polynomial time by a quantum computer, with help from a polynomial-size “quantum advice state” |n that depends only on the input size n but can otherwise be arbitrary.

How big is BQP/qpoly?

It’s not obvious why it doesn’t contain every computational problem whatsoever!

slide26

Limitations of Quantum AdviceA., 2004

Result #1: BQP/qpoly  PostBQP/poly

“Any problem you can solve using short quantum advice, you can also solve using short classical advice, provided you’re willing to use exponentially more computation time to extract what the advice is telling you.”

One can postulate bizarre, exponentially-hard-to-prepare initial states in Nature, without violating the NP Hardness Assumption

Result #2:There exists an “oracle” relative to which NP  BQP/qpoly

Evidence that NP-complete problems are still hard for quantum computers in the presence of quantum advice

slide27

Concluding Remarks

COMPUTATIONAL COMPLEXITY

THIS BRIDGE

ALREADY EXISTS

PHYSICS

Prediction: NP Hardness Assumption will eventually be seen as analogous to Second Law of Thermodynamics or impossibility of superluminal signaling

Open Question: What is polynomial time in quantum gravity?

(First question: What is time in quantum gravity?)

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