W. M. Keck Observatory · Keck II · First light on the horizon

Exoplanet spectroscopy at the diffraction limit.

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.

0.98 – 2.46 µm, single shot R > 100,000 < 30 cm s⁻¹ internal RV AO-fed · single-mode fibers
scroll — the light path awaits
01Concept

A high-resolution spectrograph built with a high-contrast imaging and interferometric front end.

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.

The RSPEC and BSPEC cryostat vessels standing together in the integration high bay
No longer a rendering — the RSPEC (red) and BSPEC (blue) vessels in the integration lab, 2026.

Four bands · one exposure

y≈ 1.0 µm · BSPEC
J≈ 1.25 µm · BSPEC
H≈ 1.6 µm · RSPEC
K≈ 2.2 µm · RSPEC

Arm coverage — BSPEC 0.98 – 1.33 µm · RSPEC 1.49 – 2.46 µm · R > 100,000 on average across both, in a single exposure.

Keck II + AO→ FEI · fiber injection→ FIB · 65 m fiber run→ CAL · wavelength references→ BSPEC + RSPEC→ H4RG-10 detectors→ DRP · spectra & RVs
02Science

Four techniques, spanning the exoplanet phase space.

Each is unlocked by the same combination: high spectral resolution, broad simultaneous coverage and a diffraction-limited fiber feed.

The HISPEC science phase space: companion mass versus semi-major axis for a simulated nearby population, overlaid with the regimes of Doppler discovery, combined-light spectroscopy, fiber nulling and high-contrast spectroscopy
The HISPEC science phase space — a simulated nearby companion population against the instrument's observing regimes. Diamonds mark benchmark systems (TRAPPIST-1 e, 51 Eri b, AF Lep b, HR 8799 d/e); circled letters, solar-system analogs at 10 pc.
Illustration of a star wobbling under the pull of an orbiting planet

Precision radial velocity

Weighing worlds around cool stars & brown dwarfs

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.

A planet in transit: a dark disk crossing the star surrounded by a translucent atmosphere annulus, with the transmission spectrum it imprints

Combined-light spectroscopy

Transits, eclipses & phase-resolved spectra

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.

The star's diffraction rings and speckle field with a single-mode fiber placed on a faint companion, whose spectrum shows H₂O, CH₄ and CO bands

High-contrast direct spectroscopy

Spectra of imaged companions

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.

Fringe pattern illustrating fiber nulling: the star on a dark fringe, the planet on a bright fringe

Fiber nulling

Inside the inner working angle

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.

Beyond exoplanets

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.

  • Galactic Center — S-star RVs from ~10 km/s to < 100 m/s: orbits, spin, tests of gravity
  • Ultracool dwarfs — spectral binaries, rotation & magnetic fields via Zeeman-sensitive K I and FeH lines
  • Milky Way & beyond — young clusters, bulge & halo abundances, dwarf-galaxy kinematics, AGN environs
  • Solar System — high-resolution infrared spectroscopy of planets, moons and comets
Illustration of the Galactic Center: highly eccentric S-star orbits sharing a focus at Sgr A*, drawn as a black disc ringed by a faint accretion glow within the dense nuclear star cluster; a dashed single-mode-fiber aperture encircles one orbiting star with a radial-velocity arrow along its orbit, annotated RV below 100 m/s
The Galactic Center — the fiber placed on an S star; radial velocities to < 100 m/s turn the orbits around Sgr A* into probes of the black hole and of gravity itself

Planning an observation? Explore sensitivities with the HISPEC exposure time calculator at specsim.astro.caltech.edu/hispec_snr · source code on GitHub.

03Specifications

Top-level requirements.

ParameterValue
TelescopeW. M. Keck II (10 m), Nasmyth platform, behind the upgraded HAKA AO
Spectral coverage0.98 – 2.46 µm (y J H K), simultaneous single-shot
Resolving power> 100,000 on average · BSPEC ≈ 150,000 · RSPEC ≈ 100,000
ChannelsBSPEC 0.98 – 1.33 µm · RSPEC 1.49 – 2.46 µm
Fiber feedSingle-mode · ~65 m · silica (yJ) + ZBLAN fluoride (HK)
Injection modesOn-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 calibration2 Fabry–Pérot astro-etalons · 2 laser frequency combs · gas cells · U/Ne lamp
Science detectors2 × Teledyne H4RG-10, < 7 e⁻ read-noise requirement
Acquisition & tracking5″-diameter field of view · H2RG infrared camera · up to 1 kHz tip/tilt sensing · ≤ 2 mas RMS
Data productsRaw UTR → L0 → L1 → L2 · quick-look ≤ 2 min · archived at KOA
04Team

The institutions behind HISPEC.

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.

World map with dots marking the HISPEC contributing institutions in Southern California, Tucson, Evanston, Greenbelt, Montréal and Tokyo, with arcs converging on Maunakea, the instrument's destination at the W. M. Keck Observatory

California Institute of Technology

Pasadena, California

Project Leads · FEI · FIB · ICS Lead

University of California Los Angeles

Los Angeles, California

SPEC · ELEC Lead

University of California San Diego

La Jolla, California

Project Science · CAL & DRP Lead

W. M. Keck Observatory

Maunakea, Hawaiʻi

GSE Lead

Jet Propulsion Laboratory

Pasadena, California

RV Error Budget · FEI Design

Astrobiology Center · NINS

Tokyo, Japan

Echelle Gratings · Fiber Switchers

NASA Goddard Space Flight Center

Greenbelt, Maryland

H4RG Detectors for the Spectrometers

University of Arizona

Tucson, Arizona

H2RG Tracking Camera Detector

Université de Montréal

Montréal, Canada

Consulting

Northwestern University

Evanston, Illinois

DRP Contributions

Co-Principal InvestigatorsDimitri MAWET (Caltech) · Michael FITZGERALD (UCLA)
Project ScientistQuinn KONOPACKY (UCSD)
Project ManagerRob BERTZ (Caltech)
Program ManagerMarc KASSIS (WMKO)
Instrument ArchitectNemanja JOVANOVIC (Caltech)
Instrument ScientistAshley BAKER (Caltech)
Systems EngineerJocelyn FERRARA (Caltech)

The team

The full instrument and science team — engineers, scientists, technicians, postdocs and students, past and present.

View the full team · 116 names
Caltech (42)

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

UCLA (12)

Björn Benneke · Ben Calvin · Therese Cook · Tuan Do · Michael Fitzgerald · Rose Gibson · Takeru Hayashi · Christopher Johnson · Charlie Kirkpatrick · Evan Kress · Kenneth Magnone · Eric Wang

UCSD (8)

Aaron Brown · Adam Burgasser · Bryson Cale · Aidan Gibbs · Quinn Konopacky · Jerome Maire · Jean-Baptiste Ruffio · Ben Sappey

W. M. Keck Observatory (12)

Matthew Brown · Greg Doppmann · Charlotte Guthery · Grant Hill · Sonia Karkar · Marc Kassis · Scott Lilley · Eduardo Marin · Jonathan Steiner · Jim Thorne · Ed Wetherell · Truman Wold

JPL (5)

Charles Beichman · Sam Halverson · Tiffany Kataria · Garreth Ruane · Gautam Vasisht

Astrobiology Center · NINS (4)

Takayuki Kotani · Norio Narita · Aoi Takahashi · Motohide Tamura

Université de Montréal (3)

Étienne Artigau · René Doyon · David Lafrenière

Northwestern University (1)

Jason Wang

Science Team · Worldwide (29)

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.

05The light path

From telescope to detectors.

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.

W. M. KECK OBSERVATORY · KECK II Maunakea · 4,145 m target dome summit level secondary 36-segment primary tertiary Nasmyth platform Keck II AO HAKA upgrade FEI TIB · trunk interface fiber conduit · ~65 m · silica yJ + ZBLAN HK observatory basement · stabilized laboratory main switchers thermal enclosure BSPEC · yJ RSPEC · HK CAL racks calibration light injected at SPEC or at the FEI Nasmyth focus DRP spectra · RVs 1 2 3 4 5 6 7 8
06Subsystems

Subsystems — status, mid-2026.

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.

Annotated CAD of the FEI bench showing the beam path from the FEI pickoff through the ADC, fast steering mirror, mask selector, filter wheel, CSD, PIAA optics and fiber coupling lenses to the fiber alignment mechanisms, with the tracking camera overhead
The FEI bench — pickoff, ADC, fast steering mirror, mask selector, PIAA optics and fiber coupling, with the tracking camera overhead
The as-built FEI inside its enclosure at Caltech, optics and fiber routing visible
The FEI as built, in its enclosure at Caltech
FEI · Front-End Instrument

Injecting a point source into a few microns of glass

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.

  • Throughput 57–62 % measured y–K — beats the 55 % spec
  • Coupling 68.7 / 73.0 % (y / H) — PIAA boost, near theory
  • ≤ 2 mas RMS tip/tilt — FSM + tracking camera
  • ADC + mask selector — wide-band correction, nulling
Labeled CAD of the HISPEC fiber route: from the Keck AO bench on the Nasmyth platform, down the telescope structure, along the Coude tunnel, to the basement with the HISPEC spectrographs, main switches rack, calibration racks and HK LFC bench
The ~65 m fiber route — Keck AO bench → telescope structure → Coude tunnel → basement spectrographs, switch rack and calibration racks
A closed FIB mechanical fiber switcher unit on its sliding rack tray
Mechanical switcher — Subaru-IRD heritage, Japanese collaboration
FIB · Fiber Transport

Sixty-five meters, summit to basement

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.

  • < 2 % loss per connector on the science bundles
  • ZBLAN HK fiber meets its 65 m transmission requirement
  • 48 switches (26 silica + 22 ZBLAN) received & tested
  • 3-port photonic lantern — > 90 % throughput, y & J
The BCAL and RCAL calibration racks with components labeled: gas cells and lamp, etalon sources, temperature controllers, and the BCAL and RCAL etalons
The BCAL (yJ) & RCAL (HK) racks, annotated — installed at Palomar Observatory for on-sky validation
CAL · Calibration

The backbone of centimeter-per-second velocimetry

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.

  • 0.14 – 0.34 m s⁻¹ etalon uncertainty per order (H / J)
  • 2 LFCs + 2 etalons · gas cells · U/Ne hollow-cathode lamp
  • Racks integrated — on sky at Palomar for validation
  • Dual injection points — spectrometer and front end
Ray trace through the RSPEC optical train: collimator box, R4 echelle grating with orders 59 to 97, cross-disperser grating with orders minus 2 to plus 2, and the camera box
RSPEC optical train — collimator, R4 echelle (orders 59–97), cross-disperser (−2 … +2) and camera
The gold-coated R4 echelle grating beside a ruler
Gold-coated R4 echelle
Electron micrograph of the echelle grating grooves at 500 times magnification
Grating grooves · SEM ×500
SPEC · Two Spectrometers

Cryogenic echelles on Invar

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.

  • All optics & cryostats fabricated — integration under way
  • R4 echelle — single-crystal Ge, direct-ruled by Canon, gold-coated · 13 nm rms WFE · 96 % of theoretical diffraction efficiency
  • Invar-36 benches · TMA collimator & camera
  • PT-60 cryocoolers · MLI · active radiation-shield control
A Teledyne H4RG-10 science array on its handling fixture, sensor face up
A Teledyne H4RG-10 — an engineering-grade spare from NASA’s Roman Space Telescope
CAD of the detector head assembly: the focal plane in its mount with copper thermal strapping and cold head
Detector head assembly — focal plane, mount and thermal strapping (CAD)
DET · Detectors & Readout

From photons to spectra

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.

  • 2 × H4RG-10 arrays at Caltech — < 7 e⁻ noise spec
  • ATC: 13 e⁻ CDS · QE 80 % · 75 K · 1 kHz windows
  • ATC cold since July 2025 — final characterization
  • Science-cryostat verification — fall 2026
Diagram of the HISPEC data reduction pipeline: raw up-the-ramp reads processed by stage 0 into rate maps, stage 1 into 1D spectra, and stage 2 into calibrated spectra and radial velocities
Raw UTR reads → L0 rate maps → L1 spectra → L2 calibrated spectra & RVs
DRP · Data Reduction Pipeline

From 3.2 TB of raw reads to radial velocities

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.

  • Quick-look L2 in ≤ 2 min of readout — goal 10 s
  • ML ramp fitting — ~9.5 % over least squares
  • 3 fibers × 40 + 39 orders extracted per exposure
  • Full processing < 24 h — products archived at KOA
Simplified HISPEC software architecture: computers hosting mKTL keyword-layer services with daemons and clients for mechanical control, monitoring, calibration, thermal control and user interfaces, plus per-spectrometer detector target systems and the FEI real-time system, all linked by the observatory-wide mKTL messaging layer
ICS overview — computers host mKTL services; daemons, clients and keyword layers communicate over the observatory-wide mKTL bus
CAD layout of the HISPEC installation in the Keck basement: electronics racks and calibration sources along the wall, the thermal enclosure with the two spectrometer cryostats, and overhead cable trays and glycol lines
Basement layout at WMKO — ELEC racks and CAL sources alongside the thermal enclosure, with cable trays and services overhead
ICS · ELEC · GSE

Control software, electronics & ground support

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.

  • mKTL architecture — daemons, clients & keyword layers on an observatory-wide bus
  • ICS EPR passed — April 2025
  • ELEC — rack-mounted control & readout electronics, summit and basement
  • GSE — utilities (power, glycol cooling) · carts, cranes & handling fixtures at WMKO
07Timeline

Integration under way, first light late 2027.

What happens next, subsystem by subsystem.

FEI

  • Fiber co-alignment with retro-beacons
  • Automated calibration scripts
  • Fast pointing control · full-system lab I&T

FIB

  • HK coupling-loss spot checks
  • 1000+-cycle switch endurance tests & control software
  • Trunk Interface Box build · end-to-end tests with FEI and SPEC

CAL

  • Continue on-sky validation at Palomar
  • Integration with BSPEC and RSPEC
  • Long-term drift monitoring of both etalons

SPEC & Detectors

  • Cold alignment and optical testing of both benches
  • H4RG-10 verification in the science cryostats — fall 2026
  • Detector readout & software integration

DRP

  • Automation framework — priority event queues at WMKO
  • Prefect-based workflow orchestration under evaluation
  • End-to-end benchmarking on simulated UTR data
The HISPEC integration lab at Caltech Cahill, with the red RSPEC and blue BSPEC vessels surrounded by team members closing out fabrication
Closing out fabrication — RSPEC and BSPEC in the HISPEC integration lab, Caltech Cahill
08Selected publications

The HISPEC literature, 2019 – present.

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.