(Symmetric) Private Information Retrieval

Description

Private information retrieval (PIR) is a classical cryptographic functionality that allows one party (user) to privately retrieve an element from a classical database owned by another party (server), i.e., without revealing to the other party which element is being retrieved (user privacy).

Symmetric private information (SPIR) retrieval is PIR with the additional requirement that throughout and after the protocol, the user remains oblivious to other database elements, i.e., apart from the queried one (data privacy).

In the quantum setting, the use of quantum systems is allowed to achieve (S)PIR: this may imply the use of a quantum channel between the user and the server, and the capability to prepare quantum states, apply quantum gates or measure quantum systems by one or both parties. (S)PIR in this setting is known as quantum (symmetric) private information retrieval (Q(S)PIR).

In the classical or quantum setting, (Q)SPIR and one-out-of-n (quantum) oblivious transfer (OT) are similar cryptographic tasks; the only minor difference between those functionalities is that protocols for OT are two-party protocols, while attempts at achieving SPIR have considered both two-party and multi-party protocols where the user communicates with several servers, each holding a copy of the database.

Apart from using quantum techniques to enhance the classical (S)PIR functionality (i.e., design better protocols than their classical counterparts in terms of different metrics like e.g., communication complexity), there has also been a recent interest in a ‘fully’ quantum (S)PIR where a user wants to query a quantum database (items are quantum states)[1].

Tags: Two Party Protocol, Specific Task, Quantum Enhanced Classical Functionality.

Properties

Security definitions

(Quantum) private information retrieval protocols are said to be secure if they satisfy the following conditions:

• Correctness: assuming that all the parties in the protocol are honest, then the output of the protocol on the user’s side must be the queried database element.
• User privacy: assuming that the user is honest, then, throughout the protocol, any query of the user to a server leaks no information about the desired database item.

In addition to the above requirements, symmetric (quantum) private information retrieval protocols must also satisfy the following condition:

• Data(base) privacy: assuming that the server(s) is (are) honest(s), then, throughout the protocol, the user is unable to obtain any information beyond a single database element.

Cost parameters

The most common cost parameter used to characterise a given (Q)(S)PIR protocol is:

• Communication complexity: total number of (qu)bits exchanged between the user and the server(s) throughout the protocol.

For (Q)(S)PIR protocols in general:

• (Q)(S)PIR capacity: maximal achievable ratio of the retrieved database element size to the total download size.

Some less common cost parameters include:

• Storage overhead (for multi-database (Q)(S)PIR protocols): ratio between the total number of (qu)bits stored on all servers and the number of (qu)bits in the (resp. quantum) classical database.
• Access complexity: total amount of data to be accessed by the server(s) for answering queries throughout a (Q)(S)PIR protocol.

Protocols

Classical database

In the quantum setting, protocols aiming at achieving (S)PIR for a classical database fall into two main categories:

Single-database protocols

As in the classical setting, in the case of the database being owned by a single server, the trivial solution (downloading the whole database) is the only way to achieve information-theoretically secure PIR – even in the case of a specious (may deviate from the protocol if its malicious operations are unknown to the user) server [2].
As for (quantum or classical) SPIR, it is impossible to achieve information-theoretic security with a single-server; this result was proved in the quantum setting by Lo [3]. Intuitively, this comes from the fact that the (unique) trivial solution of information-theoretically secure PIR is the worst in terms of data privacy. Therefore, to design efficient PIR protocols or to achieve SPIR, several assumptions have been considered; they include:

• Hardness assumptions: PIR protocols with computational security.
• Assumptions on the adversarial model:
  • to achieve SPIR: cheat-sensitive protocols (also known as quantum private queries (QPQ) protocols) where it is assumed that the server will not cheat if there is a non-zero probability that he will be caught cheating.
    • QPQ protocols based on quantum oblivious key distribution
    • QPQ protocols based on quantum random access memory
  • to achieve efficient PIR: assuming an honest server.
    • QPIR protocols in the honest server model
• Prior shared entanglement between server and user: in the honest server model, efficient PIR protocols exist, however for a specious or malicious server, the trivial solution is optimal for PIR[4].
  • QPIR protocols with prior shared entanglement in the honest server model
• Relativistic assumptions: quantum SPIR protocols whose security uses properties from special relativity.
  • Relativistic QOT protocols

Multi-database protocols

It is possible to achieve information-theoretic (S)PIR with reduced communication complexity (i.e., compared to this of the trivial solution) by considering several servers instead of one, each holding a copy of the database, and with the help of extra assumptions. Usually, to achieve (S)PIR, it is assumed that the servers cannot communicate with each other during and after the protocol ended (no-communication assumption), and that servers share randomness (in the symmetric case only). Examples of such protocols are:

• Quantum multi-database SPIR protocols without shared randomness (replaced by prior shared entanglement between servers)
• Classical multi-database SPIR protocols with QKD secured classical channels
• Multi-database quantum (S)PIR protocols for communicating and colluding servers – to do without the no-communication assumption
• Multi-database quantum (S)PIR protocols for coded servers

Quantum database

For the case of a quantum database, the trivial solution of downloading the whole database is proved to be optimal for one-round QPIR, and for multi-round QPIR in the blind setting (i.e., the servers do not have a classical description of the quantum states of the database) and for the honest server model (and any other attack model)[1].

Prior shared entanglement between the user and the server allows for efficient one-server QPIR protocols in the honest server model and in the blind setting. Multi-database QSPIR protocols for a quantum database with pure states, in the visible setting (servers know a classical description of the quantum database elements) exist as shown by Song and Hayashi [1].

• Single-database quantum PIR protocols in the honest server model and in the blind setting for a quantum database
• Multi-database quantum SPIR protocols in the visible setting for a quantum database

Use-cases

Classical database

• Location-based services (to protect user location privacy).
• Queries of electronic medical records (these require decades of information confidentiality; hence security against quantum computing based attacks is necessary) or medical test reports.
• Music and film streaming (user does not want his/her tastes to be revealed to the server).
• Pay-per-view services, where the user should pay a fee to access every single database element.

Quantum (S)PIR protocols may be preferred to their classical counterparts to:

• Achieve (S)PIR with better communication complexity: this is convenient in the case of large databases.
• Achieve (S)PIR with better security: for instance, to secure classical channels as in [5].

Further Information

Optimal communication complexity of the (Q)(S)PIR problem

Below are summarised known bounds for the communication complexity of information-theoretically secure (S)PIR protocols in the classical and quantum settings, for a quantum or classical database.

• $f$ : number of database elements (quantum states in the 'fully' quantum setting)
• $m$ : total size of database elements (i.e., the sum of the sizes, in bits, of each database element)
• $d$ : dimension of the quantum states stored in the quantum database ($d=2$ if they are qubits)
• $k$ : number of servers (or equivalently of replicated databases)

Single-database case

Problem	Additional assumptions	Optimal communication complexity	Reference
Classical PIR		$\Theta (m)$	Chor et al (1995)
Classical SPIR		NA (impossible)
Quantum PIR (Classical database)	Specious server	$\Theta (m)$	Baumeler and Broadbent (2015)
	Specious server & prior entanglement	$\Theta (m)$	Aharonov et al (2019)
	Honest server	$O(poly\log(m))$	Kerenidis et al (2016)
	Honest server & prior entanglement	$O(\log(m))$	Kerenidis et al (2016)
Quantum SPIR (Classical database)		NA (impossible)	Lo (1997)
	The server will not cheat if there is a non-zero probability of being caught cheating & imperfect data privacy (the user should get at most two database items)	$O(\log(m))$	Giovannetti et al (2008)
Quantum PIR (Quantum database)	Honest server & blind setting	$\Theta (m)$	Song and Hayashi (2021)
	Honest server & visible setting	$\Theta (m)$ (for one-round)	Song and Hayashi (2021)
	Honest server & prior entanglement	$O(\log(m))$	Song and Hayashi (2021)
Quantum SPIR (Quantum database)

Multi-database case

Problem	Additional assumptions	Optimal communication complexity	Reference
Classical PIR
Classical SPIR	Servers do not communicate with each other & secure classical channels	$O(m^{\frac {1}{2k-1}}){\text{ bits}}$	Gertner et al (2000)
Quantum PIR (Classical database)
Quantum SPIR (Classical database)	Servers do not communicate with each other	$O(m^{\frac {1}{2k-1}}){\text{ bits}}+{\text{ comm. complexity of QKD}}$	Kon and Lim (2021)
	Servers do not communicate with each other & honest user & prior entanglement	$m^{O(\log \log(k)/k\log(k))}$	Kerenidis and de Wolf (2004)
Quantum PIR (Quantum database)
Quantum SPIR (Quantum database)	Servers do not communicate with each other & prior entanglement & visible setting & database contains pure qubit states	$O(f){\text{ bits}}+O(1){\text{ qubits}}+O(1){\text{ ebits}}$	Song and Hayashi (2021)
	Servers do not communicate with each other & prior entanglement & visible setting & database contains pure qudit states	$O(f){\text{ bits}}+O(d^{d}\log(d)){\text{ qubits}}+O(d^{d}\log(d)){\text{ ebits}}$	Song and Hayashi (2021)
	Servers do not communicate with each other & prior entanglement & visible setting & database contains commutative unitaries	$O(f){\text{ bits}}+O(\log(d)){\text{ qubits}}+O(\log(d)){\text{ ebits}}$	Song and Hayashi (2021)

References

1. Song and Hayashi (2021)
2. Baumeler and Broadbent (2015)
3. Lo (1997)
4. Aharonov et al (2019)
5. Kon and Lim (2021)

*contributed by Marine Demarty