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YSM Issue 93.2

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FOCUS

Physics

THE PROMISE OF TWO-COPPER-PAIR TUNNELING

BY SHOUMIK CHOWDHURY

Every day, hundreds of Yale students

take classes in Davies Auditorium and

work in the Center for Engineering,

Innovation, and Design. Likely only several

will know that just a few stories above them—

on the 4th floor of Becton Center—reside

some of the world’s most powerful quantum

computers. These devices are housed in

the Yale Quantronics Laboratory—Qulab

for short—and are operated by cooling

superconducting circuits in microwave

cavities down to millikelvin temperatures, at

which point their behavior is aptly described

by the laws of quantum mechanics.

First proposed in the 1960s by physicist

Richard Feynman, using quantum

mechanical systems (such as atoms) for

computation is not a new concept. Much of

the progress in experimentally implementing

these devices, however, has come in the last

twenty years, with superconducting circuits

(behaving as artificial atoms) emerging as a

leading platform for quantum information

processing. Unfortunately, quantum bits,

or qubits, built from these circuits are still

highly sensitive to various types of noise

from the environment. This has driven

widespread effort in the field to build better

qubits. Recently, a team of researchers at

Qulab—led by principal investigator Michel

Devoret and graduate student Clarke

Smith—designed a new type of protected

superconducting qubit that is robust at the

hardware-level against several different

noise channels.

Notions of Quantum Computing

Quantum computers are based on a

fundamentally different set of rules than

so-called classical computers—a broad

label characterizing most devices in use

today. Classical data are stored in bits,

and a single binary digit can take on two

logical values: 0 or 1. In practice, this could

be realized by the passage of current, and

the lack thereof, through a wire, or by the

magnetization state of a small region of a

hard drive. At the lowest level, under many

layers of abstraction, all classical algorithms

and operations reduce to manipulating

some pattern of bit strings from an input

state to an output state. The key takeaway

here is that bits take on definite values.

In contrast, quantum computers encode

information in the quantum states of

a system—for instance, in the states

representing the lowest two energy levels

of an atom. These two states, which we

can abstractly label as |0> and |1>, form

what is known as qubit subspace, and by

sending appropriate pulses of light to the

atom, one can perform logical operations

on the qubit. The key difference from the

classical model, however, is that we can also

form admixtures of the two states, called

superpositions, of the form α|0> + β|1>. The

outcomes of measuring such superposition

states are determined by rules of probability,

giving either |0> and |1> with probabilities

|α|2 and |β|2 respectively. While this may

seem counterintuitive, it turns out that

several classes of problems are very wellsuited

to a quantum computer that does

not have definite 0 or 1 bits. Some notable

examples include cryptography and prime

number factorization, optimization and

machine learning, and simulating quantum

mechanical systems (such as molecules) for

applications in fundamental physics and

chemistry. However, the aforementioned

sensitivity of quantum information means

that quantum computers are also more

susceptible to noise and other errors that

arise from coupling to the environment. Any

spurious interaction can lead to unwanted

changes to the desired quantum state, and

thus introduces errors into a calculation.

The fragility of quantum information has

led to what Michel Devoret describes as a

two-pronged effort in the field. “The first

approach is to discover a better method

for quantum error correction … while the

second [approach] is to design physical

qubits with better lifetimes and faster

gate operations,” Devoret said. Research

into quantum error correction (QEC)

involves finding ways to encode a logical

bit of quantum information across many

physical qubits—the benefit is then that

the information becomes more robust

to noise, being distributed non-locally

across the system. However, these kinds of

QEC protocols are often very theoretical

in nature, and the authors of the present

study chose to focus on the more tractable

18 Yale Scientific Magazine September 2020 www.yalescientific.org

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