Dark Energy Spectroscopic Instrument
The Dark Energy Spectroscopic Instrument (DESI) is a ground-based astronomical survey instrument mounted on the 4-meter Mayall telescope at Kitt Peak National Observatory in Arizona, designed to probe the nature of dark energy by measuring the redshifts of tens of millions of galaxies and quasars across 14,000 square degrees of the sky, creating a three-dimensional map of the universe extending to nearly 11 billion light-years.[1] Over its five-year primary survey, which began in May 2021, DESI uses a novel robotic fiber-positioning system with 5,000 fiber-optic positioners to capture spectra simultaneously from thousands of celestial objects per exposure, enabling precise measurements of baryon acoustic oscillations (BAO) and the growth of cosmic structure to test models of cosmic acceleration.[2] Managed by the Lawrence Berkeley National Laboratory under the U.S. Department of Energy's Office of Science, DESI represents a Stage IV dark energy experiment, building on prior surveys like the Baryon Oscillation Spectroscopic Survey (BOSS) with unprecedented scale and precision.[3] DESI's scientific mission focuses on quantifying dark energy's influence on the universe's expansion history and large-scale structure evolution, potentially revealing deviations from the standard Lambda-CDM cosmological model through analyses of redshift-space distortions and galaxy clustering.[3] Key innovations include its wide-field corrector optics for imaging faint targets up to magnitude 22.5 and a spectrograph array that resolves wavelengths from 360 to 980 nanometers, allowing classification of galaxies, quasars, and luminous red galaxies across cosmic epochs.[4] By October 2025, DESI had released the cosmology results from Data Release 2 (DR2), incorporating data from over 30 million galaxies and quasars observed over the first three years of the survey (2021–2024) and providing cosmological constraints that refine measurements of the Hubble constant and dark energy equation of state parameter w, including hints that dark energy may evolve over time.[5][6] The project involves an international collaboration of over 900 scientists from more than 70 institutions, with construction completed in 2019 after a decade of development funded by a consortium including the DOE, NSF, and international partners.[1] Early milestones include the creation of the largest 3D cosmic map in January 2022 from initial data, encompassing nearly 7 million objects, and the Early Data Release in June 2023 with spectra for nearly 2 million objects, which have already contributed to breakthroughs in understanding cosmic voids and the Lyman-alpha forest.[7][8] By late 2024, DESI had reached a milestone of 50 million spectra. DESI's observations, expected to conclude in November 2025, promise to deliver transformative insights into the universe's fate, potentially confirming or challenging the dominance of dark energy as the driver of accelerated expansion.[9][10]Overview
Instrument Description
The Dark Energy Spectroscopic Instrument (DESI) is a multi-year survey instrument mounted on the Mayall 4-meter telescope at Kitt Peak National Observatory, designed to collect optical spectra from tens of millions of galaxies and quasars.[1][11] Its core function involves measuring redshifts of these celestial objects through optical spectroscopy, allowing scientists to trace the history of cosmic expansion as shaped by dark energy.[1] One key observable in this effort is baryon acoustic oscillations (BAO), which serve as a cosmic standard ruler to gauge the universe's expansion over time.[3] DESI targets over 40 million objects, including galaxies, quasars, and stars, across 14,000 square degrees of the sky, encompassing roughly 11 billion years of cosmic history from the nearby universe to distant epochs.[2][12] The survey's main operations began in 2021 and are scheduled to continue through 2026, producing a vast three-dimensional map of the universe.[10]Location and Operations
The Dark Energy Spectroscopic Instrument (DESI) is hosted at Kitt Peak National Observatory in Arizona, USA, where it is integrated with the Nicholas U. Mayall 4-meter Telescope.[13] This site, managed by the National Optical-Infrared Astronomy Research Laboratory (NOIRLab), provides optimal conditions for ground-based astronomical observations in the northern sky.[13] The project is led by Lawrence Berkeley National Laboratory, involving over 900 scientists from more than 70 institutions worldwide.[14] DESI conducts nights-only observations, leveraging a robotic fiber positioning system to align 5,000 optical fibers across an 8-square-degree field of view on the telescope's focal plane.[15] This setup enables the simultaneous collection of spectra from up to 5,000 astronomical objects per exposure, with positioners adjusting autonomously between exposures to target new fields.[16] On-site operations involve a team of researchers coordinating nightly scheduling, data acquisition, and real-time quality checks to ensure efficient survey progress.[17] The main survey encompasses approximately 1,000 nights of observation over five years, targeting tens of millions of galaxies and quasars to map cosmic structure.[1] Spectra are obtained across a wavelength range of 360–980 nm, with resolutions varying from R ≈ 2000 at shorter wavelengths to R ≈ 5000 at longer ones.[18] Target selection for these observations integrates photometry from the Legacy Imaging Surveys.Scientific Objectives
Primary Goals
The primary scientific goals of the Dark Energy Spectroscopic Instrument (DESI) center on elucidating the nature of dark energy, which drives the accelerated expansion of the universe. A key objective is to measure the dark energy equation of state parameter w to determine whether it remains constant, as in the cosmological constant model (\LambdaCDM with w = -1), or evolves over cosmic time. This involves parameterizing w(a) = w_0 + (1 - a) w_a, where a is the scale factor, to test models of dynamical dark energy.[19] DESI aims to constrain fundamental cosmological parameters, including the matter density \Omega_m, the Hubble constant H_0 \approx 70 km/s/Mpc, and the sum of neutrino masses \sum m_\nu to a precision of 0.020 eV. These measurements will refine the cosmic energy budget—comprising approximately 5% ordinary matter, 27% dark matter, and 68% dark energy—and enable tests of neutrino mass hierarchies when combined with cosmic microwave background data.[19] To achieve these aims, DESI will probe the universe's expansion history from redshift z=0 to z=3.5, spanning the transition from matter domination to dark energy domination over the past 11 billion years, through galaxy clustering and redshift-space distortions. The instrument targets a 1% precision measurement of the baryon acoustic oscillation (BAO) scale at multiple redshifts, providing stringent constraints on distance measures like D_V(z). DESI's three-dimensional mapping of approximately 40 million galaxies and quasars facilitates these high-precision analyses.[19]Measurement Techniques
The Dark Energy Spectroscopic Instrument (DESI) employs baryon acoustic oscillations (BAO) as a primary measurement technique to probe the cosmic expansion history. BAO features arise from fossilized sound waves in the early universe's baryon-photon plasma, imprinting a characteristic comoving scale of approximately 150 Mpc that serves as a standard ruler for distance measurements.[20] By mapping the positions of galaxies and quasars in three dimensions, DESI detects this scale in the large-scale structure, enabling determinations of the angular diameter distance D_A(z) and the Hubble parameter H(z). The angular diameter distance is given by D_A(z) = (1+z)^{-1} \int_0^z \frac{c \, dz'}{H(z')}, where c is the speed of light and the integral represents the comoving transverse distance.[21] This technique yields sub-percent precision on distance ratios across redshifts $0.1 < z < 2.1, providing robust constraints on dark energy models independent of assumptions about galaxy bias.[20] DESI also measures redshift-space distortions (RSD) to infer the growth rate of cosmic structure and test general relativity on large scales. RSD occur due to the peculiar velocities of galaxies, which distort their observed positions along the line of sight relative to their real-space coordinates, enhancing clustering anisotropies in the radial direction.[21] By analyzing these distortions in galaxy samples such as luminous red galaxies and emission-line galaxies, DESI quantifies the growth rate parameter f\sigma_8(z), where f is the logarithmic derivative of the growth factor and \sigma_8 is the normalization of matter fluctuations on 8 h^{-1} Mpc scales.[20] This measurement achieves precisions of around 0.74% at effective wavenumbers up to k_{\max} = 0.1 \, h \, \mathrm{Mpc}^{-1}, offering insights into the rate at which density perturbations evolve under gravity.[21] Spectroscopic redshifts in DESI are determined through high-resolution optical spectra, with precision \sigma_z / (1+z) \sim 0.0005, enabling accurate three-dimensional positioning of targets. For quasars and emission-line galaxies, where direct template matching may be challenging due to broad emission lines or faint continua, DESI uses cross-correlation techniques with imaging surveys to refine redshift estimates.[21] This involves correlating spectroscopic samples with photometric catalogs from the Legacy Imaging Surveys, leveraging spatial clustering to calibrate mean redshifts and reduce uncertainties, particularly for high-redshift quasars (z > 2) and emission-line objects at $0.6 < z < 1.6.[1] Such methods ensure high success rates, around 72% for emission-line galaxies and 67% for quasars in single-pass observations, as measured in Data Release 1 (as of 2024).[22][23] Statistical analysis of DESI data centers on the power spectrum P(k) and the two-point correlation function \xi(r) to characterize large-scale structure and extract BAO and RSD signals. The power spectrum, the Fourier transform of \xi(r), quantifies density fluctuations as a function of wavenumber k and line-of-sight angle \mu, modeled as P(k, \mu, z) = b^2 (1 + \beta \mu^2)^2 P_m(k, z) D(k, \mu, z), where b is the galaxy bias, \beta = f/b, and P_m is the matter power spectrum.[21] The correlation function \xi(r) measures excess probability of finding galaxy pairs separated by comoving distance r, revealing the BAO peak and RSD anisotropies in configuration space.[20] These complementary tools, applied to over 30 million spectra, enable joint constraints on cosmological parameters with minimal shot noise, achieving \bar{n} P \approx 1 at relevant scales for key tracers.[21]Instrument Design
Spectrograph and Optics
The Dark Energy Spectroscopic Instrument (DESI) employs ten identical spectrographs to process light collected from 5,000 optical fibers, with each spectrograph handling 500 fibers via fiber-optic cables that integrate with the focal plane system.[24][25] These spectrographs are housed in a thermally controlled enclosure to maintain stability, enabling simultaneous acquisition of high-quality spectra over a broad wavelength range. The design prioritizes high throughput and resolution to support precise measurements of galaxy redshifts and cosmological probes. Each spectrograph divides incoming light using dichroic beamsplitters into three channels: blue (360–555 nm), red (555–656 nm), and infrared (656–980 nm). The optical train includes a collimator to parallelize the light, a volume phase holographic (VPH) grating for dispersion, and a camera lens assembly to focus the spectrum onto the detector. The blue channel achieves a spectral resolution R = \lambda / \Delta\lambda of 2,000–3,200, while the red and infrared channels reach 3,200–4,100 and 4,100–5,000, respectively, ensuring adequate separation of emission lines for target classification.[24] Detectors are 4,096 × 4,096 pixel CCDs with 15 μm pixels, cooled in cryostats to minimize noise, and the system delivers an overall throughput exceeding 70% across the operational wavelengths.[25] The wavelength coverage is optimized for key emission lines essential to DESI's science goals, including the Lyman-α forest in quasars (z ≈ 1.9–2.7) detected in the blue channel, the [O II] doublet in emission-line galaxies (z ≈ 0.5–0.8) in the red channel, and Hα in bright galaxies (z ≈ 0–0.5) in the infrared channel. Quantum efficiency of the detectors surpasses 50% across the full band, with peaks above 85% in the 600–900 nm range and over 60% beyond 900 nm, enhancing sensitivity for faint targets.[25][25] Calibration of the spectrographs relies on dedicated sky fibers and standard stars to achieve flux accuracy and minimize systematics. 20 dedicated sky fibers in total (approximately 2 per spectrograph) enable precise sky subtraction by modeling zodiacal and atmospheric emission, while 100 standard stars per field (10 per petal) provide spectrophotometric calibration, ensuring relative flux errors below 5% across the wavelength range.[26][27] Internal LED illuminators further support fiber-to-fiber throughput uniformity checks during observations.[24]Fiber Positioning System
The Fiber Positioning System of the Dark Energy Spectroscopic Instrument (DESI) features 5,020 robotic positioners arrayed across a approximately 1-meter-diameter focal plane at the prime focus of the 4-m Mayall Telescope, enabling simultaneous spectroscopy of up to 5,000 targets over a 3.2-degree field of view. Each positioner, known as a "cobra" due to its serpentine actuation mechanism, employs two independent motors—one for azimuthal rotation and one for polar elevation—to steer an optical fiber within a patrol region of roughly 12 mm in diameter. These motors, typically piezoelectric or DC brushless gear types, achieve a positioning accuracy better than 5 micrometers root-mean-square (RMS), far exceeding the <10-micrometer requirement for reliable target acquisition while minimizing focal ratio degradation in the fiber optics.[28][16] The positioners are organized in a hexapod-supported focal plane assembly, divided into 10 wedge-shaped petals with 500 positioners per petal in a dense hexagonal packing pattern averaging 10.4 mm center-to-center spacing. This configuration optimizes coverage density (about 667 fibers per square degree on-sky) while accommodating the instrument's wide-field corrector optics. Each fiber has a 107-micrometer core diameter, equivalent to 1.5 arcseconds on the sky, balancing light collection from point-like galaxies and quasars against inclusion of excess sky background. The hexapod mount provides six degrees of freedom for sub-micrometer adjustments to the entire focal plane, compensating for gravitational flexure and thermal variations to maintain alignment throughout observations.[29][30] Repositioning occurs in coordinated 30-minute cycles between exposures, with the robotic array reconfiguring all fibers in under 2 minutes to target new fields, followed by a typical 1,000-second science integration. This sequence supports DESI's high-throughput survey strategy, allowing over 376,000 total moves across the 5-year mission without significant duty-cycle loss. For redundancy in telescope pointing and focus, the system dedicates 80 guide fibers, back-illuminated for imaging by dedicated cameras, to provide real-time metrology and corrections during observations. The positioned fibers route captured light via 47.5-meter cable assemblies to the spectrographs for dispersion and detection.[16][31]Development and History
Project Origins
The Dark Energy Spectroscopic Instrument (DESI) project emerged as a response to the limitations of earlier galaxy surveys, particularly the Baryon Oscillation Spectroscopic Survey (BOSS), which demonstrated the power of baryon acoustic oscillations (BAO) for probing dark energy but required larger samples for Stage IV precision. In April 2009, the BigBOSS concept was proposed as a DOE-NSF Stage IV ground-based experiment to extend BAO measurements to higher redshifts and volumes, targeting spectra for over 20 million galaxies and quasars to achieve sub-percent accuracy on dark energy parameters. Building on this, early 2011 saw unsolicited proposals submitted to the DOE: BigBOSS, led by Lawrence Berkeley National Laboratory (LBNL), and the competing DESpec concept from Fermilab, both aiming to upgrade an existing telescope for massively multiplexed spectroscopy. In September 2012, the DOE approved the mission need (CD-0) for a merged Mid-scale DESI (MS-DESI) project and selected the Nicholas U. Mayall 4-meter Telescope at Kitt Peak National Observatory for the upgrade, citing its dark skies, accessibility, and prior NSF investment as key advantages over alternatives like the Blanco Telescope. LBNL was assigned project management in December 2012, with initial leadership from the laboratory's physics division.[32] The scientific rationale was further detailed in LBNL-led white papers, including a submission to the 2013 Snowmass Community Planning Meeting, which positioned DESI as essential for measuring the universe's expansion history and growth of structure through redshift surveys of emission-line galaxies, luminous red galaxies, and quasars.[33] Construction funding reached approximately $75 million, including $56 million from the DOE Office of Science for instrument development and telescope modifications, supplemented by NSF grants for operations and imaging support, plus contributions from international partners and private foundations. International collaborations formalized in 2014, incorporating over 70 institutions from more than 20 countries to bolster expertise in instrumentation, data analysis, and theory.[34][35] These origins paved the way for DESI's evolution into full-scale construction starting in 2015.Construction and Milestones
The construction of the Dark Energy Spectroscopic Instrument (DESI) began with major upgrades to the Nicholas U. Mayall 4-meter Telescope at Kitt Peak National Observatory, initiated in 2015 and spanning through 2019. These modifications centered on replacing the telescope's original prime focus instrumentation with a new prime focus cage and a sophisticated six-lens corrector optics system, designed to deliver a wide 3.2-degree field of view with high image quality across an 8-square-degree focal plane. The corrector, featuring lenses up to 1 meter in diameter, transformed the telescope's focal ratio from f/2.8 to f/3.8 (average over the field of view), enabling precise targeting for DESI's 5,000 robotic fiber positioners. First light for this upgraded optical system was achieved on April 1, 2019, marking a key step in integrating the instrument with the telescope.[36][37][38] Instrument assembly and integration occurred primarily at Lawrence Berkeley National Laboratory, led by the DESI collaboration under U.S. Department of Energy funding, from 2018 onward through early 2021. This phase involved fabricating and testing the core components, including the barrel assembly housing 10 spectrographs, the focal plane with its robotic positioners for fiber placement, and the extensive fiber optic system linking the telescope to the spectrographs. The positioners, each capable of sub-10-micron accuracy, underwent rigorous actuation testing to ensure reliable targeting of astronomical objects, addressing challenges in mechanical precision and thermal stability. Full instrument first light was attained on October 22, 2019, when the 5,000 fiber-optic "eyes" successfully captured spectra from the night sky, initiating on-site validation.[38][39][16] The COVID-19 pandemic introduced significant delays, halting on-site operations at Kitt Peak from March to November 2020 during the validation phase, which required remote adaptations for hardware and software testing. Commissioning resumed in December 2020 and concluded successfully by March 2021, allowing the main five-year spectroscopic survey to commence on May 17, 2021. In 2022, observations were paused from June to September due to the Contreras fire at Kitt Peak, but the project remained on track. Ongoing observations continue to build toward the survey's completion in 2026.[38][40][41]Surveys and Observations
Legacy Imaging Surveys
The Legacy Imaging Surveys consist of three complementary photometric projects designed to provide wide-field optical imaging over the northern and southern Galactic caps, serving as precursors to the Dark Energy Spectroscopic Instrument (DESI) observations. These surveys—the Dark Energy Camera Legacy Survey (DECaLS), the Mayall z-band Legacy Survey (MzLS), and the Beijing-Arizona Sky Survey (BASS)—collectively cover approximately 14,000 square degrees in the DESI footprint, with imaging in the g, r, and z bands, and additional i-band data from DECaLS.[42][43] DECaLS utilizes the Dark Energy Camera on the Blanco 4 m telescope at Cerro Tololo Inter-American Observatory, imaging the region south of declination +32° (including both north and south Galactic caps) to depths of 5σ = 24.7 mag in g, 23.9 mag in r, 23.0 mag in z, and approximately 22.5 mag in i for point sources under typical seeing conditions.[42][44] In the northern Galactic cap, BASS employs the 90Prime camera on the Steward Observatory 2.3 m Bok telescope to observe in g and r bands to 5σ depths of 24.0 mag and 23.4 mag, respectively, while MzLS uses the Mosaic-3 camera on the Nicholas U. Mayall 4 m telescope at Kitt Peak National Observatory for z-band imaging to a 5σ depth of 22.5 mag; both cover declinations ≥ +32°.[42][44] This multi-instrument approach ensures uniform depth and calibration across the DESI footprint, with data processed using the Legacy Surveys pipeline to produce catalogs of galaxies and stars via multi-wavelength forced photometry.[42] The primary purpose of these surveys is to enable photometric redshift estimation and target selection for DESI's spectroscopic program, identifying millions of objects across key classes: bright galaxies (BGS) at low redshift (z < 0.4) for large-scale structure tracing, luminous red galaxies (LRGs) at intermediate redshifts (0.4 < z < 1.0), emission-line galaxies (ELGs) at higher redshifts (0.6 < z < 1.6) via lines like [O II], and quasars (QSOs) spanning z < 2.1 for baryon acoustic oscillations and z > 2.1 for Lyman-α forest analysis.[42][45] Photometric redshifts are derived using template-fitting methods calibrated against spectroscopic samples, achieving typical accuracies of σ_z/(1+z) ≈ 0.02 for LRGs and 0.03 for ELGs, which support the selection of over 30 million spectroscopic targets.[42] These imaging data thus provide the foundational target lists that feed into DESI's fiber assignment for the main spectroscopic survey.[45] All data from the Legacy Imaging Surveys are publicly released through the NOIRLab Astro Data Archive and the dedicated Legacy Surveys portal, with the latest Data Release 10 (DR10, completed in 2023) including processed images, catalogs with over 1 billion sources, and software tools for analysis; earlier releases like DR9 covered the core DESI area.[44][46]| Survey | Instrument/Telescope | Coverage (deg²) | Filters | 5σ Depths (AB mag, point sources) |
|---|---|---|---|---|
| DECaLS | DECam/Blanco 4 m | ~9,000 (δ ≤ +32°) | g, r, z, i | g=24.7, r=23.9, z=23.0, i~22.5 |
| BASS | 90Prime/Bok 2.3 m | ~5,000 (δ ≥ +32°) | g, r | g=24.0, r=23.4 |
| MzLS | Mosaic-3/Mayall 4 m | ~5,000 (δ ≥ +32°) | z | z=22.5 |