<HashMap><database>biostudies-literature</database><scores/><additional><omics_type>Unknown</omics_type><volume>649(8096)</volume><submitter>Chen HJ</submitter><pubmed_abstract>Over the past decades, remarkable progress has been made in reducing the loss of photonic integrated circuits (PICs) within the telecom band&lt;sup>1-4&lt;/sup>, facilitating on-chip applications spanning low-noise optical&lt;sup>5&lt;/sup> and microwave synthesis&lt;sup>6&lt;/sup>, to lidar&lt;sup>7&lt;/sup> and photonic artificial intelligence engines&lt;sup>8&lt;/sup>. However, several obstacles arise from the marked increase in material absorption and scattering losses at shorter wavelengths&lt;sup>9,10&lt;/sup>, which prominently elevate power requirements and limit performance in the visible and near-visible spectrum. Here we present an ultralow-loss PIC platform based on germano-silicate-the material underlying the extraordinary performance of optical fibre-but realized by a fully CMOS-foundry-compatible process. These PICs achieve resonator Q factors surpassing 180 million from violet to telecom wavelengths. They also attain a 10-dB higher quality factor without thermal treatment in the telecom band, expanding opportunities for heterogeneous integration with active components&lt;sup>11&lt;/sup>. Other features of this platform include readily engineered waveguide dispersion, acoustic mode confinement and large-mode-area-induced thermal stability-each demonstrated by soliton microcomb generation, stimulated Brillouin lasing and low-frequency-noise self-injection locking, respectively. The success of these germano-silicate PICs can ultimately enable fibre-like loss onto a chip, leading to an additional 20-dB improvement in waveguide loss over the current highest performance photonic platforms. Moreover, the performance abilities demonstrated here bridge ultralow-loss PIC technology to optical clocks&lt;sup>12&lt;/sup>, precision navigation systems&lt;sup>13&lt;/sup> and quantum sensors&lt;sup>14&lt;/sup>.</pubmed_abstract><journal>Nature</journal><pagination>338-344</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC12779554</full_dataset_link><repository>biostudies-literature</repository><pubmed_title>Towards fibre-like loss for photonic integration from violet to near-infrared.</pubmed_title><pmcid>PMC12779554</pmcid><pubmed_authors>Gates J</pubmed_authors><pubmed_authors>Bouwmeester D</pubmed_authors><pubmed_authors>Vahala K</pubmed_authors><pubmed_authors>Liu P</pubmed_authors><pubmed_authors>Ge J</pubmed_authors><pubmed_authors>Blauvelt H</pubmed_authors><pubmed_authors>Ji QX</pubmed_authors><pubmed_authors>Chen HJ</pubmed_authors><pubmed_authors>Lehan P</pubmed_authors><pubmed_authors>Colburn K</pubmed_authors><pubmed_authors>Liu JY</pubmed_authors><pubmed_authors>Holmes C</pubmed_authors><pubmed_authors>Hou H</pubmed_authors><pubmed_authors>Yan H</pubmed_authors><pubmed_authors>Yuan Z</pubmed_authors></additional><is_claimable>false</is_claimable><name>Towards fibre-like loss for photonic integration from violet to near-infrared.</name><description>Over the past decades, remarkable progress has been made in reducing the loss of photonic integrated circuits (PICs) within the telecom band&lt;sup>1-4&lt;/sup>, facilitating on-chip applications spanning low-noise optical&lt;sup>5&lt;/sup> and microwave synthesis&lt;sup>6&lt;/sup>, to lidar&lt;sup>7&lt;/sup> and photonic artificial intelligence engines&lt;sup>8&lt;/sup>. However, several obstacles arise from the marked increase in material absorption and scattering losses at shorter wavelengths&lt;sup>9,10&lt;/sup>, which prominently elevate power requirements and limit performance in the visible and near-visible spectrum. Here we present an ultralow-loss PIC platform based on germano-silicate-the material underlying the extraordinary performance of optical fibre-but realized by a fully CMOS-foundry-compatible process. These PICs achieve resonator Q factors surpassing 180 million from violet to telecom wavelengths. They also attain a 10-dB higher quality factor without thermal treatment in the telecom band, expanding opportunities for heterogeneous integration with active components&lt;sup>11&lt;/sup>. Other features of this platform include readily engineered waveguide dispersion, acoustic mode confinement and large-mode-area-induced thermal stability-each demonstrated by soliton microcomb generation, stimulated Brillouin lasing and low-frequency-noise self-injection locking, respectively. The success of these germano-silicate PICs can ultimately enable fibre-like loss onto a chip, leading to an additional 20-dB improvement in waveguide loss over the current highest performance photonic platforms. Moreover, the performance abilities demonstrated here bridge ultralow-loss PIC technology to optical clocks&lt;sup>12&lt;/sup>, precision navigation systems&lt;sup>13&lt;/sup> and quantum sensors&lt;sup>14&lt;/sup>.</description><dates><release>2026-01-01T00:00:00Z</release><publication>2026 Jan</publication><modification>2026-06-14T06:13:36.571Z</modification><creation>2026-06-14T03:17:03.868Z</creation></dates><accession>S-EPMC12779554</accession><cross_references><pubmed>41501200</pubmed><doi>10.1038/s41586-025-09889-w</doi></cross_references></HashMap>