Rochester's qudit research asks when more quantum levels are useful
A new laboratory profile explores the control costs of a richer quantum state space.

A new Bluefors profile explores how Machiel Blok's group at the University of Rochester uses superconducting circuits with more than two accessible levels. Published on October 27, the interview focuses on qudits and the challenge of controlling their additional states.[1]
The group is investigating whether those states can represent some simulation problems more naturally. Blok describes control methods that address multiple transitions together, alongside work on noise, and laboratory training.[1]
The profile also describes the cryogenic infrastructure supporting the experiments. Because it is published by a supplier, equipment claims should remain attributed. The piece does not establish a new independent performance record or a general advantage over -based computers.[1]
Editorial interpretation
The useful question is when a richer local system reduces the cost of a complete task. More available levels also create more transitions to calibrate and more behavior to characterize. Readers should look for workload-specific evidence that the representation gains survive those practical control requirements.
Learn: Count control effort alongside qudit states
A qudit uses a quantum system with more than two available basis states. That additional structure may represent some problems more directly. Whether it helps a computation depends on how accurately and efficiently those states can be prepared, manipulated and measured.
The first comparison is mathematical. A four-level system has the same state-space dimension as two two-level systems. That statement is about dimension. It does not establish that their available operations, error behavior or readout costs are interchangeable. It also does not mean a measurement reveals every amplitude of the state.[1]
Worked example
Hypothetical example: an algorithm needs 20 control pulses in one four-level implementation and 40 pulses in a two-level implementation. Counting pulses alone favors the first design. If the assumed pulses last 2 microseconds in the first system and 0.5 microseconds in the second, the totals become 40 and 20 microseconds. These invented values show why a smaller operation count does not settle the timing comparison.
Accuracy adds another layer. The comparison should ask whether unwanted population enters other levels, whether the required states can be distinguished during readout and how reliably operations connect the intended transitions. Those tests need to reflect the actual algorithm rather than an isolated best-performing transition.
Higher dimensions still have a clear appeal. If a physical problem naturally uses several states, a direct representation may simplify its mapping. The useful question is whether that simpler mapping survives the cost of control and correction.
Readers should look for results normalized to the same task and output accuracy. Device count, pulse count, execution time and success probability can then be considered together. This gives qudit research credit for what it demonstrates while leaving room for different encodings to be effective for different problems.