Scattering and quantum information

In high energy and gravitational physics, the S-matrix is the starting point for studying any fundamental physics in asymptotically flat spacetimes. In the context of information theory, the S-matrix can be viewed simply as one of many possible unitary time evolution operators. I'll give some simple examples highlighting the overlap of these views; in particular, I will discuss the interplay of entanglement with relativistic scattering.

Truly quantum Gibbs: Thermal state of a system whose charges don’t commute

The grand canonical ensemble lies at the core of statistical mechanics. A small system thermalizes to this state while exchanging heat and particles with a bath. A quantum system may exchange quantities, or “charges,” represented by operators that fail to commute. Whether such a system thermalizes, and what form the thermal state has, concerns truly quantum thermodynamics.
 

What does the Moser-Tardos RESAMPLE algorithm do when it does not work?

The celebrated Lovasz Local Lemma (LLL) guarantees that locally sparse systems always have solutions, which one can also algorithmically find by the Moser-Tardos RESAMPLE algorithm. Among the major questions that remain open is  that  how far *beyond* Lovasz's condition can we expect that RESAMPLE still performs in polynomial (linear) expected running time? Stating the question correctly is a challenge already. For a solvable and fixed instance RESAMPLE always comes up with a solution, but the catch is that the number of steps may be very large.

Zero-knowledge proof systems for QMA

Zero-knowledge (ZK) proof systems are fundamental in modern cryptography. Prior work has established that all problems in NP admit classical zero-knowledge proof systems, and under reasonable hardness assumptions for quantum computations, these proof systems can be made secure against quantum attacks.

 

Quantum-security of commitment schemes and hash functions

Commitment schemes are a fundamental primitive in cryptography. Their security (more precisely the computational binding property) is closely tied to the notion of collision-resistance of hash functions. Classical definitions of binding and collision-resistance turn out too be weaker than expected when used in the quantum setting. We present strengthened notions (collapse-binding commitments and collapsing hash functions), explain why they are "better", and show how they be realized under standard assumptions.

What information theory teaches us on gravitational theory

Positive energy theorems play a fundamental role in general relativity. Recently, we found a new class of positive energy theorems using information inequalities such as the positivity and monotonicity of the relative entropy.

This and related applications of information theory are providing us new insights into gravitational theory.

 

Unifying gate-synthesis and magic state distillation

The leading paradigm for performing computation on quantum memories can be encapsulated as distill-then-synthesize. Initially, one performs several rounds of distillation to create high-fidelity magic states that provide one good T-gate, an essential quantum logic gate. Subsequently, gate synthesis intersperses many T-gates with Clifford gates to realise a desired circuit. We introduce a unified framework that implements one round of distillation and multi-qubit gate synthesis in a single step.

Quantum circuits for quantum operations

Every quantum gate can be decomposed into a sequence of single-qubit gates and controlled-NOTs. In many implementations, single-qubit gates are relatively 'cheap' to perform compared to C-NOTs (for instance, being less susceptible to noise), and hence it is desirable to minimize the number of C-NOT gates required to implement a circuit.