W. M. Keck Observatory · Keck II · First light on the horizon
HISPEC is a single-mode-fiber-fed infrared spectrograph for the Keck II telescope, recording y, J, H and K simultaneously at a resolving power above 100,000 on average.
HISPEC feeds any point-like source — a star, a brown dwarf, or a directly imaged planet — into single-mode fibers at the diffraction limit of Keck II. Behind Keck II’s newly upgraded HAKA adaptive optics — a 2844-actuator ALPAO deformable mirror and an OCAM²K EMCCD wavefront-sensor camera, upgrades that underpin HISPEC’s efficiency and high-contrast reach — a compact front end, heir to the KPIC pathfinder, injects the corrected beam into fibers only a few microns across. That choice sets everything else: a pristine, telescope-independent line-spread function, an instrument compact enough to stabilize deeply, and direct access to high-contrast techniques like cross-aperture fiber nulling.
The fibers carry the light ~65 meters down to a stabilized basement laboratory, where two cryogenic echelle spectrometers — BSPEC (y+J) and RSPEC (H+K) — disperse the full 0.98–2.46 µm range in a single exposure at R > 100,000. A dedicated dual-channel calibration system — astro-etalons tracked continuously, laser frequency combs, gas cells and lamps — pins the wavelength solution at the precision the science demands.
The same fiber-fed architecture is designed to scale to a 30-meter aperture — a future TMT instrument concept known as MODHIS.
Each is unlocked by the same combination: high spectral resolution, broad simultaneous coverage and a diffraction-limited fiber feed.
Precision radial velocity
Sub-m s⁻¹ infrared velocimetry — calibrated against Fabry–Pérot etalons and a laser frequency comb — weighing temperate planets around M dwarfs and brown dwarfs. Observed simultaneously with KPF in the optical, it disentangles stellar jitter around Sun-like stars too.
Combined-light spectroscopy
Resolving thousands of lines as a planet transits, is eclipsed, or rotates through its orbit — escaping He I at 1.083 µm, the K I doublets, FeH and other refractories, then H₂O, CH₄, NH₃, CO and CO₂ toward K band — from hot Jupiters toward ice giants, mini-Neptunes, super-Earths, and Earth-like planets in favorable cases.
High-contrast direct spectroscopy
Fibers placed directly on faint companions reject the stellar speckle field, enabling high-dispersion characterization — H₂O, CO and CH₄ abundances, spins, winds — and the radial velocity of the planet itself, opening a search for exomoons.
Fiber nulling
A pupil phase mask (vortex or phase knife) nulls the on-axis star while a companion's light couples into the fiber — reaching separations at and inside λ/D. A natural follow-up for Gaia astrometric candidates: detection and spectral characterization in a single observation.
Exoplanets drive the design, but a stable R > 100,000 spectrograph at the diffraction limit of Keck reaches well beyond them. The flagship case is the Galactic Center: today’s AO spectrographs measure the S stars orbiting Sgr A* to roughly 10 km/s in radial velocity — HISPEC sharpens that by two orders of magnitude. At < 100 m/s, the stellar orbits become precision probes of the black hole: its mass, its spin through the drag of nearby space-time, general relativity in the strongest gravity we can observe, limits on an intermediate-mass companion, and even whether the fine-structure constant drifts in such extreme environments.
Planning an observation? Explore sensitivities with the HISPEC exposure time calculator at specsim.astro.caltech.edu/hispec_snr · source code on GitHub.
| Parameter | Value |
|---|---|
| Telescope | W. M. Keck II (10 m), Nasmyth platform, behind the upgraded HAKA AO |
| Spectral coverage | 0.98 – 2.46 µm (y J H K), simultaneous single-shot |
| Resolving power | > 100,000 on average · BSPEC ≈ 150,000 · RSPEC ≈ 100,000 |
| Channels | BSPEC 0.98 – 1.33 µm · RSPEC 1.49 – 2.46 µm |
| Fiber feed | Single-mode · ~65 m · silica (yJ) + ZBLAN fluoride (HK) |
| Injection modes | On-axis · off-axis companion · fiber nulling |
| Point-source sensitivity | ~15 mag (Vega) · S/N > 30 per spectral resel in 4 h |
| Radial-velocity precision | < 30 cm s⁻¹ internal error budget |
| Wavelength calibration | 2 Fabry–Pérot astro-etalons · 2 laser frequency combs · gas cells · U/Ne lamp |
| Science detectors | 2 × Teledyne H4RG-10, < 7 e⁻ read-noise requirement |
| Acquisition & tracking | 5″-diameter field of view · H2RG infrared camera · up to 1 kHz tip/tilt sensing · ≤ 2 mas RMS |
| Data products | Raw UTR → L0 → L1 → L2 · quick-look ≤ 2 min · archived at KOA |
HISPEC is led from Caltech, with the spectrometers built at UCLA and the calibration system at UCSD, working alongside the W. M. Keck Observatory, JPL and Northwestern. The Astrobiology Center (NINS, Japan) contributed the echelle gratings and the robotic fiber switchers, and Université de Montréal provides scientific and technical consulting. The H4RG detectors for the spectrometers are provided by NASA’s Goddard Space Flight Center, and the H2RG for the tracking camera by the University of Arizona — engineering-grade devices from the Roman Space Telescope and JWST programs, respectively.
Pasadena, California
Project Leads · FEI · FIB · ICS Lead
Los Angeles, California
SPEC · ELEC Lead
La Jolla, California
Project Science · CAL & DRP Lead
Maunakea, Hawaiʻi
GSE Lead
Pasadena, California
RV Error Budget · FEI Design
Tokyo, Japan
Echelle Gratings · Fiber Switchers
Greenbelt, Maryland
H4RG Detectors for the Spectrometers
Tucson, Arizona
H2RG Tracking Camera Detector
Montréal, Canada
Consulting
Evanston, Illinois
DRP Contributions
The full instrument and science team — engineers, scientists, technicians, postdocs and students, past and present.
Elijah Anakalea-Buckley · Jeb Bailey · Ashley Baker · Rob Bertz · Geoffrey Blake · David Brearley · James Brugger · Richard Dekany · Daniel Echeverri · Jocelyn Ferrara · Luke Finnerty · Jason Fucik · Thomas Greene · Prakriti Gupta · Michael Gutierrez · David Hale · Lynne Hillenbrand · Katelyn Horstman · Andrew Howard · Nemanja Jovanovic · Heather Knutson · Michael Langmayr · Andrea Lin · Larry Lingvay · Dimitri Mawet · Ricardo Meneses · Reston Nash · Don Neill · Alberto Ordovás · Rishi Pahuja · Michael Porter · Bradley Price · Reed Riddle · Mitsuko Roberts · Aniket Sanghi · Gregory Sercel · Roger Smith · Tatum Umiamaka · Bob Weber · James Wiley · Ray Zarzaca · Jake Zimmer
Björn Benneke · Ben Calvin · Therese Cook · Tuan Do · Michael Fitzgerald · Rose Gibson · Takeru Hayashi · Christopher Johnson · Charlie Kirkpatrick · Evan Kress · Kenneth Magnone · Eric Wang
Aaron Brown · Adam Burgasser · Bryson Cale · Aidan Gibbs · Quinn Konopacky · Jerome Maire · Jean-Baptiste Ruffio · Ben Sappey
Matthew Brown · Greg Doppmann · Charlotte Guthery · Grant Hill · Sonia Karkar · Marc Kassis · Scott Lilley · Eduardo Marin · Jonathan Steiner · Jim Thorne · Ed Wetherell · Truman Wold
Charles Beichman · Sam Halverson · Tiffany Kataria · Garreth Ruane · Gautam Vasisht
Takayuki Kotani · Norio Narita · Aoi Takahashi · Motohide Tamura
Étienne Artigau · René Doyon · David Lafrenière
Jason Wang
David Anderson (TMT International Observatory) · Thomas Beatty (University of Wisconsin–Madison) · Gabriela Canalizo (UC Riverside) · Guo Chen (Purple Mountain Observatory, CAS) · Courtney Dressing (UC Berkeley) · Min Fang (Purple Mountain Observatory, CAS) · Greg Herczeg (Peking University) · Stephen Kane (UC Riverside) · Eliza Kempton (University of Maryland) · Stephanie Leifer (The Aerospace Corporation) · Chao Liu (NAOC, CAS) · Stanimir Metchev (Western University) · Max Millar-Blanchaer (UC Santa Barbara) · Shogo Nishiyama (Miyagi University of Education) · Gajendra Pandey (Indian Institute of Astrophysics) · Peter Plavchan (George Mason University) · S. P. Rajaguru (Indian Institute of Astrophysics) · Paul Robertson (UC Irvine) · Colette Salyk (Vassar College) · Bun'ei Sato (Tokyo Institute of Technology) · Everett Schlawin (Schmidt Sciences) · Sujan Sengupta (Indian Institute of Astrophysics) · Thirupathi Sivarani (Indian Institute of Astrophysics) · Warren Skidmore (TMT International Observatory) · Hiroshi Terada (TMT International Observatory) · Ji Wang (Ohio State University) · Chikako Yasui (TMT International Observatory) · Hui Zhang (Shanghai Astronomical Observatory, CAS) · Huihao Zhang (Ohio State University)
Supported by the Caltech fund for Keck instrumentation, the Gordon and Betty Moore Foundation, the Heising-Simons Foundation, W. M. Keck Observatory and the University of California Observatories, with in-kind contributions from NASA, the Astrobiology Center (NINS) and Northwestern University.
Light from the target — a star, or a planet beside one — is corrected on the Nasmyth platform, threaded into single-mode fibers, and carried down through the telescope building to a stabilized laboratory beneath the dome floor. Select any station along the path.
The subsystems are materializing — benches populated, cryostats delivered, fibers terminated — and the data-reduction pipeline is coming to life on real detector data. A snapshot of where each stands, Summer 2026.
On the Nasmyth platform behind the upgraded HAKA AO, the FEI acquires the target, stabilizes it with a fast steering mirror and infrared tracking camera, reshapes the beam with PIAA optics, and couples it into single-mode fibers — on-axis, on a faint companion, or through a nulling mask.
Light arrives through the FEI pickoff and meets a compact train: an atmospheric dispersion corrector keeps all four bands stacked on the fiber tip, the fast steering mirror closes its loop against the tracking camera overhead, and a selector wheel drops pupil masks — including the nulling masks — into the beam. PIAA lenses then remold Keck’s segmented pupil into a near-Gaussian beam before the coupling lenses and fiber alignment mechanisms take over.
An internal light source and retro-illuminated fiber beacons let the whole chain be aligned and calibrated without touching the sky — the key to fast, automated target acquisition once the unit is installed behind HAKA.
A ~65 m run of single-mode fibers carries the light from the Nasmyth focus down to the basement: silica for y and J, custom ZBLAN fluoride fiber for H and K. Mechanical switchers — carrying Subaru-IRD heritage from the Japanese collaboration — plus MEMS switchyards and a photonic lantern reconfigure science, sky and calibration paths.
Every connection is engineered to stay pristine over thousands of reconfigurations: the sealed, pressure-regulated switcher units carry their own stick-cleaner banks, an inspection microscope and 3D-printed fiber guides inside. From the Nasmyth platform, the bundles thread the telescope’s cable wraps and the Coude tunnel before landing at the trunk interface box in the basement lab.
Two laser frequency combs, gas absorption cells and a U/Ne hollow-cathode lamp anchor the absolute wavelength solution, while two astro-etalons track drift continuously. Split into BCAL (yJ) and RCAL (HK), the references inject at the spectrometers or all the way up at the front end — tracing the full optical path.
Each rack pairs an absolute reference with a continuous one: the frequency combs and lamps pin the wavelength solution, while temperature-stabilized etalons — kept under vacuum by ion pumps, held by precision temperature controllers and cooled through a glycol heat exchanger — track instrumental drift between comb exposures. Running on sky at Palomar against PARVI is retiring the risk long before the racks reach Maunakea.
Split at the FEI dichroic upstairs, the yJ and HK channels arrive on separate fibers at BSPEC and RSPEC in the basement laboratory: each an Invar-36 bench carrying a three-mirror-anastigmat collimator and camera, a gold-coated R4 single-crystal germanium echelle and a cross-disperser — cooled by a PT-60 cryocooler behind multi-layer insulation and an actively controlled radiation shield.
Inside each vessel the fiber outputs are collimated by a three-mirror anastigmat, dispersed by the echelle — orders 59 to 97 in RSPEC — cross-dispersed by a −2 to +2-order grating, and reimaged by a matching TMA camera onto the detector. Everything bolts to an Invar-36 bench on G10 A-frames, thermally isolating the optics inside the gold-shielded vacuum space.
Each camera focuses the cross-dispersed orders onto a Teledyne H4RG-10 — an engineering spare from the Roman Space Telescope — read through light-tight feedthroughs by Archon controllers. Up front, a JWST-heritage H2RG tracking camera closes the tip/tilt loop at up to 1 kHz.
The two science arrays were characterized side by side before installation — 4.95 and 7.02 e⁻ CDS read noise, 93 and 99 % quantum efficiency for the BSPEC and RSPEC devices — sampled up the ramp for jump-free, low-noise integrations. The tracking camera is a small instrument in its own right: a four-channel H2RG behind a cold snout and K-blocking filter, windowing on the target at up to 1 kHz over its 6″ field.
The Python pipeline turns raw up-the-ramp detector reads into science-ready spectra and radial velocities in three stages — with a calibration database synced to the Keck Observatory Archive and quick-look feedback in the dome while you observe.
Stage 0 alone runs a full detector-calibration chain — saturation and jump detection, bias, reference-pixel and 1/f correction, non-linearity, dark, gain and flat — before the maximum-likelihood ramp fit turns each read cube into a rate map. Downstream, wavelength solutions accurate to tens of m/s, simultaneous-etalon drift correction and telluric treatment deliver spectra ready for cross-correlation radial velocities.
Behind the optics sits the infrastructure. The instrument control software (ICS) is an mKTL-based layer of daemons, clients and keyword services spanning motion, monitoring, calibration, thermal control and detectors — reviewed at its engineering peer review in April 2025. The electronics (ELEC) power and interface every mechanism from racks at the summit and in the basement, and the ground support equipment (GSE) covers the utilities — power and glycol cooling — together with the servicing infrastructure at the observatory: carts, cranes, lifting and handling fixtures, and the basement layout itself.
The HISPEC concept is born — a diffraction-limited, fiber-fed infrared spectrograph for Keck II.
CoDR passed — the architecture is set: AO-fed single-mode injection, a ~65 m fiber run, and two cryogenic echelle arms in the basement.
PDR passed at Caltech — the gate into construction, assessing designs, cost and schedule for the remaining work.
Subsystem MRRs passed ahead of fabrication: CAL (UCSD, Nov 2023), FEI (Caltech, May 2024), SPEC (UCLA, Oct 2024) and FIB (Caltech, Nov 2024).
EPRs passed for the software subsystems: DRP (UCSD, Dec 2024) and the instrument control software (Caltech, Apr 2025).
Held at UCLA after all subsystem MRRs — budget and schedule for the remainder of the project reviewed and confirmed, with FEI fabrication just underway.
Cryostat vessels delivered; ATC detector installed in its cryostat; fiber bundles drawn and terminated; CAL racks assembled.
FEI exceeds its throughput requirement; CAL is validating on sky at Palomar; 48 fiber switches tested; spectrometer benches populated.
The front end ships to the summit for installation behind the upgraded HAKA AO.
PSR — the gate to ship HISPEC from Caltech to WMKO — then spectrometers, calibration system and fiber runs installed, with end-to-end integration on the mountain.
Commissioning on sky — and the start of HISPEC science operations.
OHR assesses deployment and documentation status for long-term support of the instrument at the observatory.
The public HISPEC literature — the founding white paper, the science-case study, and the SPIE instrumentation papers describing each subsystem. Proceedings from the 2026 SPIE meeting will be added as they appear on arXiv.