Deuterated silicon nitride on 8-inch wafers puts a broadband light source inside the fab
A Singapore team swapped hydrogen for deuterium in silicon nitride, cut loss to 0.54 dB per centimeter, and spanned 1.7 octaves. The sub-400 C process is the part fabs will care about.
The Scientist · Science desk

What happened
- A Singapore team led by SUTD's Dawn Tan and A*STAR IME's Luo Xianshu built a low-loss silicon nitride waveguide that generates broadband light on a chip.
- Growing the film from deuterated silane moves the absorbing bond's peak out of the telecom band to the 2.1 micron region, removing the need for high-temperature annealing.
- An 800-nanometer film went down in a single deposition step below 400 degrees Celsius across a full 8-inch wafer.
- The waveguides lose 0.54 decibels per centimeter, enough headroom for a 5.21-centimeter device to drive spectral broadening.
- 500-femtosecond pulses at 1,555 nanometers came out as a continuum from 587 to 1,883 nanometers, a span of 1.7 octaves.
Why it matters
- capability Because the film never sees a temperature that would kill transistors, this kind of source can be layered onto wafers that already carry electronics rather than fabricated separately.
- constraint The absorbing bond was relocated, not removed, so pushing the same platform further into the mid-infrared runs at a band that was not in the way before.
- cost About 2.8 dB is lost over the device length, so roughly half the launched light never reaches the output and the pump laser pays for the length the nonlinearity requires.
- decision Instrument builders specifying a supercontinuum source now have a chip on a production-format wafer to weigh against a fiber module, and the comparison is on volume and power draw.
The absorption that spoils ordinary silicon nitride comes from silicon-hydrogen bonds left over from the silane the film is grown from, and they sit at the wavelengths telecommunications systems use [5]. Vibrational frequencies scale with the mass of the atoms doing the vibrating, so putting deuterium in place of hydrogen moves the absorption rather than eliminating it; Tan says the peak lands in the 2.1 micron region [7]. That bargain has a visible edge. The long-wavelength end of the continuum stops roughly 217 nm short of the relocated absorption peak [17]. The account available does not say the deuterium band sets that limit, but anyone extending this platform deeper into the mid-infrared is now heading toward an absorption feature instead of away from one.
The spectral claim is at least self-consistent. A span from 587 to 1,883 nm is a frequency ratio of 3.21, or 1.68 octaves [18], which matches the reported 1.7 and the statement that light at one end oscillates more than three times faster than at the other [10]. The chip also glowed red under an input that was itself invisible [11], which is the cheapest available demonstration that infrared went in and visible came out.
The binding constraint here was never breadth, it was thickness. Nonlinear broadening wants a thick film, and the conventional route makes transparency and thickness fight each other: hours at up to 1,200 C to drive off the hydrogen, which builds enough stress into a thick film to crack it and would destroy any transistor sharing the wafer [6]. That combination is why silicon nitride supercontinuum has stayed outside standard semiconductor factories [12].
Provenance is doing real work in this result. The fabrication sits with A*STAR IME's silicon photonics department, whose head describes the hard part as translating the photonic design into a process that delivers the required optical performance at wafer scale [13]. A wafer-scale claim owned by a foundry process group is a different object from the same claim out of a university cleanroom, and it is the reason the 8-inch figure carries weight rather than decoration.
Breadth alone does not buy a frequency comb. The light has to be coherent and repeatable from pulse to pulse [15], and the material available reports a coherence measurement at moderate pulse energies without stating the value. That number, at the energies needed for the full span, is what the metrology case rests on. Fiber-based systems already produce the spectrum; the first author frames the unmet need as compact, energy-efficient and integrable sources [14], which is a claim about form factor and power, not about optics [3].
What to watch
- The spectral coherence figure at the pulse energies needed for the full 1.7-octave span, which the available account leaves out.
- Loss and spectrum measured die to die across a whole 8-inch wafer, which is what a manufacturability claim actually rests on.
- Whether deuterated silane supply and price hold at production volume, and whether the 2.1 micron band caps mid-infrared reach.
Clarity's read
What the record supports and how the coverage leans. The claims behind it follow.
Reality
- Evidence66
- Adoption
- Insufficient
- Hype gap+18
- Incentives55
- Confidence60
Claim ledger
Ranked by verification strength, evidence, and original report placement.
- [1]
A Singapore research team led by Associate Professor Dawn Tan of the Singapore University of Technology and Design and Dr Luo Xianshu, head of the Silicon Photonics Department at A*STAR Institute of Microelectronics, developed a low-loss silicon nitride waveguide that generates broadband light on a chip.
- [2]
The work was published in Optics Express as "Octave-spanning supercontinuum generation in a wafer-scale, low loss deuterated silicon nitride waveguide".
- [3]
Today's supercontinuum sources are mostly built around specially engineered optical fiber, which is bulky, power-hungry and difficult to shrink onto a chip.
- [4]
Supercontinuum light underpins high-resolution medical imaging, precision measurement and the frequency combs used in optical clocks.
- [5]
Silicon nitride films are typically grown from silane gas, leaving silicon-hydrogen bonds that absorb light at precisely the wavelengths telecommunications systems use.
- [6]
Purging silicon-hydrogen bonds requires hours of annealing at up to 1,200 degrees Celsius, a temperature no chip carrying electronic circuitry could survive, and one that builds crippling stress into thick films.
- [7]
Tan says replacing hydrogen with deuterium moves the absorption peak from the telecommunications range to the 2.1 micron region, so the high-temperature baking process is no longer necessary.
- [8]
An 800-nanometer-thick film was deposited in a single step at below 400 degrees Celsius across a full 8-inch wafer, within the thermal budget of standard semiconductor lines and the format used in mainstream chip manufacturing.
- [9]
The finished waveguides lose 0.54 decibels of light per centimeter, low enough for a 5.21-centimeter device to sustain the optical interactions that spectral broadening demands.
- [10]
500-femtosecond infrared pulses at 1,555 nanometers were broadened into a continuum stretching from 587 to 1,883 nanometers, a span of 1.7 octaves, meaning light at one end oscillates more than three times faster than at the other.
- [11]
Although the input light was infrared and invisible, red light could be seen glowing from the chip.
- [12]
Making silicon nitride transparent enough demands conditions so extreme that thick films crack, and standard semiconductor factories cannot accommodate the process.
- [13]
Luo said the key challenge was translating the photonic design into a process that could deliver the required optical performance at wafer scale, combining SUTD's nonlinear photonics expertise with A*STAR IME's process development and fabrication capabilities.
- [14]
Yao Wang, doctoral student and first author, said the primary gap is the need for compact, energy-efficient and integrable light sources, and that fiber-based systems are standard but bulky and not easily integrated onto chips.
- [15]
For metrology and frequency comb applications the light must also be coherent, stable and repeatable from pulse to pulse; the team measured an overall spectral coherence at moderate pulse energies.
- [16]
At 0.54 dB/cm over 5.21 cm, end-to-end propagation loss is about 2.81 dB, meaning roughly 52 percent of the launched light reaches the output before any coupling losses.
- [17]
The 1,883 nm long-wavelength edge of the continuum falls about 217 nm short of the relocated absorption peak near 2.1 microns.
- [18]
A 587 to 1,883 nm span is a frequency ratio of 3.21, or 1.68 octaves, consistent with the reported 1.7 octaves and the more-than-threefold frequency statement.
Sources
1 independent publisher whose own reporting we read for this story.
- phys.orgDeuterium enables chip waveguides to generate broadband light from infrared pulses
1 article · August 24, 2026
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