<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Pages | FINER</title><link>https://finerreceiver.github.io/page/</link><atom:link href="https://finerreceiver.github.io/page/index.xml" rel="self" type="application/rss+xml"/><description>Pages</description><generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>en-us</language><lastBuildDate>Sat, 03 Jun 2023 18:21:00 +0000</lastBuildDate><image><url>https://finerreceiver.github.io/media/sharing.jpg</url><title>Pages</title><link>https://finerreceiver.github.io/page/</link></image><item><title>Publications</title><link>https://finerreceiver.github.io/publications/</link><pubDate>Sat, 03 Jun 2023 18:21:00 +0000</pubDate><guid>https://finerreceiver.github.io/publications/</guid><description>&lt;h2 id="instrument-papers">Instrument papers&lt;/h2>
&lt;ul>
&lt;li>Kang, H., Kojima, T., Sakai, T., Tamura, Y., Ishii, S., et al. 2026, &amp;ldquo;A Wideband Millimeter-wave Receiver at 210–350 GHz for LMT-FINER&amp;rdquo;, Proc. SPIE, &lt;a href="https://arxiv.org/abs/2606.25637" target="_blank" rel="noopener">arXiv:2606.25637&lt;/a>&lt;/li>
&lt;li>Taniguchi, A., Tamura, Y., Sakai, T., Hagimoto, M., Hashimoto, T., et al. 2026, &amp;ldquo;FINER: development of the wideband millimeter-wave receiver system and preparations for first light on the Large Millimeter Telescope&amp;rdquo;, Proc. SPIE, &lt;a href="https://arxiv.org/abs/2607.03265" target="_blank" rel="noopener">arXiv:2607.03265&lt;/a>&lt;/li>
&lt;li>Tamura, Y., Sakai, T., Kawabe, R., Kojima, T., Taniguchi, A., et al. 2024, &amp;ldquo;FINER: Far-Infrared Nebular Emission Receiver for the Large Millimeter Telescope&amp;rdquo;, Proc. SPIE, 13102, 131020G, &lt;a href="https://doi.org/10.1117/12.3017788" target="_blank" rel="noopener">doi:10.1117/12.3017788&lt;/a>, &lt;a href="https://arxiv.org/abs/2406.07975" target="_blank" rel="noopener">arXiv:2406.07975&lt;/a>&lt;/li>
&lt;li>Kang, H., et al. 2024, &amp;ldquo;Development status of wideband millimeter-wave receivers for LMT-FINER&amp;rdquo;, Proc. SPIE, 13102, 131020J, &lt;a href="https://doi.org/10.1117/12.3018190" target="_blank" rel="noopener">doi:10.1117/12.3018190&lt;/a>, &lt;a href="https://arxiv.org/abs/2406.07974" target="_blank" rel="noopener">arXiv:2406.07974&lt;/a>&lt;/li>
&lt;li>Hagimoto, M., Taniguchi, A., et al. 2024, &amp;ldquo;A 10.24-GHz-wide digital spectrometer array system for LMT-FINER: system design and laboratory performance verification&amp;rdquo;, Proc. SPIE, 13102, 131020V, &lt;a href="https://doi.org/10.1117/12.3018296" target="_blank" rel="noopener">doi:10.1117/12.3018296&lt;/a>, &lt;a href="https://arxiv.org/abs/2406.07978" target="_blank" rel="noopener">arXiv:2406.07978&lt;/a>&lt;/li>
&lt;/ul>
&lt;h2 id="b4r-the-precursor-of-finer">B4R, the precursor of FINER&lt;/h2>
&lt;ul>
&lt;li>Yonetsu, T., Kawabe, R., Yoshimura, Y., Taniguchi, K., Shimajiri, Y., et al. 2025, &amp;ldquo;The LMT 2 millimeter receiver system (B4R). II. Science demonstration observations toward Orion-KL/OMC-1&amp;rdquo;, &lt;a href="https://arxiv.org/abs/2511.21845" target="_blank" rel="noopener">arXiv:2511.21845&lt;/a>&lt;/li>
&lt;li>Kawabe, R., Sakai, T., Tanaka, K., Taniguchi, A., Hatsukade, B., Tamura, Y., et al. 2025, &amp;ldquo;The LMT 2 Millimeter Receiver System (B4R). I. Overview and Results of Science Demonstration&amp;rdquo;, AJ, 170, 350, &lt;a href="https://doi.org/10.3847/1538-3881/ae12eb" target="_blank" rel="noopener">doi:10.3847/1538-3881/ae12eb&lt;/a>&lt;/li>
&lt;/ul>
&lt;h2 id="sis-mixer-technology">SIS mixer technology&lt;/h2>
&lt;ul>
&lt;li>Kojima, T., et al. 2020, A&amp;amp;A, 640, L9 (&lt;a href="https://ui.adsabs.harvard.edu/abs/2020A%26A...640L...9K/" target="_blank" rel="noopener">ADS&lt;/a>)&lt;/li>
&lt;li>Kojima, T., et al. 2017, IEEE Trans. Terahertz Sci. Technol., 7, 694 (&lt;a href="https://ui.adsabs.harvard.edu/abs/2017ITTST...7..694K/" target="_blank" rel="noopener">ADS&lt;/a>)&lt;/li>
&lt;/ul></description></item><item><title>FAQ</title><link>https://finerreceiver.github.io/faq/</link><pubDate>Thu, 06 Apr 2023 16:26:33 +0000</pubDate><guid>https://finerreceiver.github.io/faq/</guid><description>&lt;h3 id="how-can-i-use-finer">How can I use FINER?&lt;/h3>
&lt;p>FINER will be offered on the LMT through the regular &lt;a href="http://lmtgtm.org/for-lmt-users/call-for-proposals/?lang=en" target="_blank" rel="noopener">LMT Call for Proposals&lt;/a> after commissioning. Observing time on the LMT is allocated to the LMT partner communities, and eligibility to propose follows the rules of each Call; there is currently no formal route for proposers outside the LMT partnership.&lt;/p>
&lt;h3 id="when-does-finer-come-online">When does FINER come online?&lt;/h3>
&lt;p>FINER is expected to come online in 2027, after installation and commissioning on the LMT.&lt;/p>
&lt;h3 id="can-i-join-finer-development">Can I join FINER development?&lt;/h3>
&lt;p>Yes. We welcome new collaborators in the development of FINER. Please contact the PI, Yoichi Tamura (Nagoya University; ytamura (at) nagoya-u.jp).&lt;/p></description></item><item><title>Receiver</title><link>https://finerreceiver.github.io/receiver/</link><pubDate>Thu, 06 Apr 2023 16:26:29 +0000</pubDate><guid>https://finerreceiver.github.io/receiver/</guid><description>&lt;h2 id="specifications">Specifications&lt;/h2>
&lt;p>FINER is a dual-polarization, sideband-separating (2SB) SIS receiver system. The table below summarizes the configuration installed for first light and the design goals of the full system.&lt;/p>
&lt;table>
&lt;thead>
&lt;tr>
&lt;th>General&lt;/th>
&lt;th>&lt;/th>
&lt;/tr>
&lt;/thead>
&lt;tbody>
&lt;tr>
&lt;td>Number of bands&lt;/td>
&lt;td>2 (one band observed at a time at first light)&lt;/td>
&lt;/tr>
&lt;tr>
&lt;td>Number of beams per band&lt;/td>
&lt;td>1&lt;/td>
&lt;/tr>
&lt;tr>
&lt;td>Number of polarizations per band&lt;/td>
&lt;td>2&lt;/td>
&lt;/tr>
&lt;tr>
&lt;td>Number of sidebands per band&lt;/td>
&lt;td>2 (2SB)&lt;/td>
&lt;/tr>
&lt;/tbody>
&lt;/table>
&lt;table>
&lt;thead>
&lt;tr>
&lt;th>&lt;/th>
&lt;th>Band 4 (first light)&lt;/th>
&lt;th>Band 6+7&lt;/th>
&lt;th>Band 4+5 (planned upgrade)&lt;/th>
&lt;/tr>
&lt;/thead>
&lt;tbody>
&lt;tr>
&lt;td>Radio frequency&lt;/td>
&lt;td>≈138–178 GHz&lt;/td>
&lt;td>≈210–351 GHz&lt;/td>
&lt;td>120–210 GHz&lt;/td>
&lt;/tr>
&lt;tr>
&lt;td>Intermediate frequency (per sideband, per polarization)&lt;/td>
&lt;td>4–8 GHz&lt;/td>
&lt;td>4–20 GHz&lt;/td>
&lt;td>4–20 GHz&lt;/td>
&lt;/tr>
&lt;tr>
&lt;td>Receiver noise temperature (SSB, design goal)&lt;/td>
&lt;td>—&lt;/td>
&lt;td>75 K&lt;/td>
&lt;td>45 K&lt;/td>
&lt;/tr>
&lt;/tbody>
&lt;/table>
&lt;p>Measured performance will be reported here after commissioning on the LMT.&lt;/p>
&lt;h2 id="system-overview">System overview&lt;/h2>
&lt;p>At first light FINER has two front-end receivers in a single cryostat: a Band 4 MMIC receiver and a wideband Band 6+7 receiver, both developed at NAOJ. A wideband Band 4+5 receiver covering 120–210 GHz is planned as a later upgrade. IF switches select which band feeds the four IF chains, so one band is observed at a time; simultaneous dual-band observation is an option for a future optics upgrade.&lt;/p>
&lt;p>
&lt;figure >
&lt;div class="d-flex justify-content-center">
&lt;div class="w-100" >&lt;img alt="blockdiagram" srcset="
/receiver/blockdiagram_hu8988208362343374286.webp 400w,
/receiver/blockdiagram_hu12044572305927477874.webp 760w,
/receiver/blockdiagram_hu12156292723166870635.webp 1200w"
src="https://finerreceiver.github.io/receiver/blockdiagram_hu8988208362343374286.webp"
width="760"
height="343"
loading="lazy" data-zoomable />&lt;/div>
&lt;/div>&lt;/figure>
&lt;strong>Figure. Block diagram of the full FINER system (design).&lt;/strong>&lt;/p>
&lt;h3 id="optics">Optics&lt;/h3>
&lt;p>The FINER warm optics picks off the beam after the LMT&amp;rsquo;s M4 mirror with a pair of motorized mirrors (the &amp;ldquo;periscope&amp;rdquo;), which can be set and stowed remotely. A chopper with a blackbody load is used for intensity calibration. A fast sky chopper for quick position switching is planned in a later phase. The spatial resolution (PSF size) is about 7 arcsec × (frequency / 200 GHz)&lt;sup>−1&lt;/sup>.&lt;/p>
&lt;h3 id="front-end-receivers">Front-end receivers&lt;/h3>
&lt;p>The front-end receivers exploit the high critical current density SIS mixer technology developed for the ALMA Wideband Sensitivity Upgrade (WSU) (&lt;a href="https://ui.adsabs.harvard.edu/abs/2017ITTST...7..694K/" target="_blank" rel="noopener">Kojima et al. 2017&lt;/a>, &lt;a href="https://ui.adsabs.harvard.edu/abs/2020A%26A...640L...9K/" target="_blank" rel="noopener">2020&lt;/a>; &lt;a href="https://arxiv.org/abs/2606.25637" target="_blank" rel="noopener">Kang et al. 2026&lt;/a>), which provides a wide instantaneous frequency coverage.&lt;/p>
&lt;h3 id="back-end-spectrometers">Back-end spectrometers&lt;/h3>
&lt;ul>
&lt;li>&lt;strong>Wideband spectrometers (DRS4, ELECS Inc.).&lt;/strong> Two DRS4 chassis digitize eight 10.24 GHz-wide basebands with 3-bit, 20.48 GSa/s analog-to-digital converters and provide spectra with 20 MHz resolution (&lt;a href="https://doi.org/10.1117/12.3018296" target="_blank" rel="noopener">Hagimoto et al. 2024&lt;/a>). Sideband separation is also performed digitally.&lt;/li>
&lt;li>&lt;strong>High-resolution spectrometers (XFFTS, RPG).&lt;/strong> The XFFTS spectrometers of the LMT 2-mm receiver B4R (2.5 GHz bandwidth, 88 kHz resolution) remain available for high-resolution spectroscopy.&lt;/li>
&lt;/ul>
&lt;h3 id="data-and-software">Data and software&lt;/h3>
&lt;p>FINER is controlled from the LMT Telescope Control System. The data format and the reduction pipeline are being developed together with the LMT team.&lt;/p>
&lt;h2 id="technical-documents">Technical documents&lt;/h2>
&lt;table>
&lt;thead>
&lt;tr>
&lt;th>Document&lt;/th>
&lt;th>Version&lt;/th>
&lt;th>Download&lt;/th>
&lt;/tr>
&lt;/thead>
&lt;tbody>
&lt;tr>
&lt;td>FINER proposal to the LMT&lt;/td>
&lt;td>Version A, 15 June 2023&lt;/td>
&lt;td>&lt;a href="https://finerreceiver.github.io/files/FINER_Proposal_verA.pdf">PDF (5 MB)&lt;/a>&lt;/td>
&lt;/tr>
&lt;/tbody>
&lt;/table>
&lt;p>The proposal describes the original design and plan; the configuration and schedule have since been updated as described on this page.&lt;/p>
&lt;h2 id="references">References&lt;/h2>
&lt;p>See &lt;a href="../publications/">Publications&lt;/a> for the instrument papers.&lt;/p></description></item><item><title>Science</title><link>https://finerreceiver.github.io/science/</link><pubDate>Thu, 06 Apr 2023 16:26:23 +0000</pubDate><guid>https://finerreceiver.github.io/science/</guid><description>&lt;h2 id="galaxy-formation-in-the-first-half-of-the-epoch-of-reionization">Galaxy formation in the first half of the epoch of reionization&lt;/h2>
&lt;h3 id="background">Background&lt;/h3>
&lt;p>The James Webb Space Telescope (JWST) has found more than a hundred candidate galaxies at redshifts &lt;em>z&lt;/em> &amp;gt; 8, when the Universe was less than about 600 million years old, and has confirmed some of them spectroscopically out to &lt;em>z&lt;/em> ≈ 14. The bright end of their ultraviolet luminosity function evolves surprisingly little with redshift (&lt;a href="https://ui.adsabs.harvard.edu/abs/2022ApJS..259...20H/abstract" target="_blank" rel="noopener">Harikane et al. 2022&lt;/a>), which means that massive galaxies had to grow very efficiently within a short time. This places a stringent constraint on models of cosmic structure formation.&lt;/p>
&lt;p>To understand what drives this rapid growth, we need spectroscopy that answers two questions:&lt;/p>
&lt;ul>
&lt;li>How common are bright, massive galaxies in the early epoch of reionization (their number density)?&lt;/li>
&lt;li>What physical conditions control their growth (metallicity, ionization state and gas density)?&lt;/li>
&lt;/ul>
&lt;h3 id="far-infrared-nebular-emission-lines">Far-infrared nebular emission lines&lt;/h3>
&lt;p>The far-infrared fine-structure line of doubly ionized oxygen, [O III] 88 µm, was proposed as a powerful tracer for identifying the redshifts of the most distant galaxies (&lt;a href="https://ui.adsabs.harvard.edu/abs/2014ApJ...780L..18I/abstract" target="_blank" rel="noopener">Inoue et al. 2014&lt;/a>). ALMA observations of this line revealed extremely high [O III]/[C II] ratios, indicating highly ionized gas filling these young galaxies (&lt;a href="https://ui.adsabs.harvard.edu/abs/2016Sci...352.1559I/abstract" target="_blank" rel="noopener">Inoue et al. 2016&lt;/a>), and held the record for the most distant spectroscopic redshift obtained with ALMA until 2022 (&lt;a href="https://ui.adsabs.harvard.edu/abs/2018Natur.557..392H/abstract" target="_blank" rel="noopener">Hashimoto et al. 2018&lt;/a>). Even in the JWST era, [O III] 88 µm at &lt;em>z&lt;/em> &amp;gt; 9 is as detectable as the rest-frame ultraviolet lines observed with JWST/NIRSpec.&lt;/p>
&lt;p>However, ALMA in the southern hemisphere cannot easily observe high-declination fields. Many bright galaxies at &lt;em>z&lt;/em> &amp;gt; 8 found in northern deep fields, such as GOODS-North and CEERS, remain unexplored in the far-infrared lines (Figure 1).&lt;/p>
&lt;p>
&lt;figure >
&lt;div class="d-flex justify-content-center">
&lt;div class="w-100" >&lt;img alt="Bright galaxies at z &amp;gt; 8 in the northern sky remain unexplored with ALMA" srcset="
/science/fig_bright_unexplored_hu13425632865376482023.webp 400w,
/science/fig_bright_unexplored_hu15657293127650879742.webp 760w,
/science/fig_bright_unexplored_hu9735927736208423550.webp 1200w"
src="https://finerreceiver.github.io/science/fig_bright_unexplored_hu13425632865376482023.webp"
width="760"
height="372"
loading="lazy" data-zoomable />&lt;/div>
&lt;/div>&lt;/figure>
&lt;strong>Figure 1.&lt;/strong> UV absolute magnitude versus spectroscopic redshift of galaxies at &lt;em>z&lt;/em> &amp;gt; 6. Green and blue circles are galaxies with and without ALMA detections; red crosses are galaxies in northern fields. Adapted from &lt;a href="https://ui.adsabs.harvard.edu/abs/2025ApJ...980..138H/abstract" target="_blank" rel="noopener">Harikane et al. 2025, ApJ, 980, 138&lt;/a> (colour coding by M. Hagimoto).&lt;/p>
&lt;h3 id="key-science-goals">Key science goals&lt;/h3>
&lt;p>With FINER on the 50-m LMT in Mexico (latitude 19°N), we aim to:&lt;/p>
&lt;ul>
&lt;li>identify the spectroscopic redshifts of bright galaxies at &lt;em>z&lt;/em> ≈ 8–15 in the northern sky using [O III] 88 µm and [C II] 158 µm, including galaxies confirmed by JWST and photometric candidates from wide-field surveys such as &lt;em>Euclid&lt;/em> and &lt;em>Roman&lt;/em>;&lt;/li>
&lt;li>detect [O III] 88 µm from a bright Lyman break galaxy in a single night of observation;&lt;/li>
&lt;li>measure the number density of bright galaxies in the first half of the epoch of reionization and diagnose their interstellar medium.&lt;/li>
&lt;/ul>
&lt;h3 id="how-finer-helps">How FINER helps&lt;/h3>
&lt;p>A typical photometric redshift uncertainty of Δ&lt;em>z&lt;/em> ≈ 1 at &lt;em>z&lt;/em> ≈ 10 requires a spectral coverage of more than 30 GHz to find the line. FINER covers about 38 GHz in a single tuning, whereas the current ALMA needs four or more tunings for the same range (Figure 2). Combined with 40% of ALMA&amp;rsquo;s collecting area and a high-altitude site (4,600 m), this offers the most sensitive spectral-scanning capability among millimeter and submillimeter telescopes in the northern hemisphere (Figure 3).&lt;/p>
&lt;p>
&lt;figure >
&lt;div class="d-flex justify-content-center">
&lt;div class="w-100" >&lt;img alt="Redshift identification with ALMA and FINER" srcset="
/science/fig_redshift_id_hu14634751317202249282.webp 400w,
/science/fig_redshift_id_hu14155497282478871541.webp 760w,
/science/fig_redshift_id_hu5294646385052334832.webp 1200w"
src="https://finerreceiver.github.io/science/fig_redshift_id_hu14634751317202249282.webp"
width="760"
height="359"
loading="lazy" data-zoomable />&lt;/div>
&lt;/div>&lt;/figure>
&lt;strong>Figure 2.&lt;/strong> The [O III] 88 µm line of the &lt;em>z&lt;/em> = 8.31 galaxy MACS0416_Y1 was found after four ALMA tunings (&lt;a href="https://ui.adsabs.harvard.edu/abs/2019ApJ...874...27T/abstract" target="_blank" rel="noopener">Tamura et al. 2019&lt;/a>). The orange bars show the frequency range FINER covers in a single tuning (19 GHz × 2 sidebands).&lt;/p>
&lt;p>
&lt;figure >
&lt;div class="d-flex justify-content-center">
&lt;div class="w-100" >&lt;img alt="Expected line intensities and FINER sensitivity" srcset="
/science/fig_finer_sensitivity_hu11221714991053659958.webp 400w,
/science/fig_finer_sensitivity_hu5097370986278833971.webp 760w,
/science/fig_finer_sensitivity_hu12783330082050089209.webp 1200w"
src="https://finerreceiver.github.io/science/fig_finer_sensitivity_hu11221714991053659958.webp"
width="760"
height="552"
loading="lazy" data-zoomable />&lt;/div>
&lt;/div>&lt;/figure>
&lt;strong>Figure 3.&lt;/strong> Expected [O III] 88 µm and [C II] 158 µm flux densities of a bright Lyman break galaxy (&lt;em>M&lt;/em>&lt;sub>UV&lt;/sub> = −21.5) at &lt;em>z&lt;/em> = 8–15, compared with the minimum 5σ-detectable flux density of LMT-FINER in 10 hours (gray). The bars in the inset compare the instantaneous IF bandwidths of FINER and the current ALMA (&lt;a href="https://arxiv.org/abs/2406.07975" target="_blank" rel="noopener">Tamura et al. 2024&lt;/a>).&lt;/p>
&lt;h2 id="further-science-cases">Further science cases&lt;/h2>
&lt;p>FINER also offers unique capabilities for a broad range of science, including:&lt;/p>
&lt;ul>
&lt;li>the Solar System (planetary atmospheres and comets),&lt;/li>
&lt;li>the interstellar medium and astrochemistry,&lt;/li>
&lt;li>star formation,&lt;/li>
&lt;li>nearby galaxies,&lt;/li>
&lt;li>distant dusty star-forming galaxies, including spectroscopic follow-up of galaxies detected with TolTEC.&lt;/li>
&lt;/ul>
&lt;p>See the &lt;a href="https://finerreceiver.github.io/files/FINER_Proposal_verA.pdf">FINER proposal (PDF)&lt;/a> for details.&lt;/p></description></item></channel></rss>