8×10-17 fractional laser frequency instability with a long room-temperature cavity

Sebastian Häfner; Stephan Falke; Christian Grebing; Stefan Vogt; Thomas Legero; Mikko Merimaa; Christian Lisdat; Uwe Sterr

doi:10.1364/OL.40.002112

8×10^-17 fractional laser frequency instability with a long room-temperature cavity

Sebastian Häfner^*
, Stephan Falke
, Christian Grebing
, Stefan Vogt
, Thomas Legero
, Mikko Merimaa
, Christian Lisdat
, Uwe Sterr

^*Corresponding author for this work

Research output: Contribution to journal › Article › Scientific › peer-review

284 Citations (Scopus)

Abstract

We present a laser system based on a 48 cm long optical glass resonator. The large size requires a sophisticated thermal control and optimized mounting design. A self-balancing mounting was essential to reliably reach sensitivities to acceleration of below Δν/ν < 2 × 10^-10/g in all directions. Furthermore, fiber noise cancellations from a common reference point near the laser diode to the cavity mirror and to additional user points (Sr clock and frequency comb) are implemented. Through comparison with other cavity-stabilized lasers and with a strontium lattice clock, instability of below 1 × 10^-16 at averaging times from 1 to 1000 s is revealed.

Original language	English
Pages (from-to)	2112-2115
Number of pages	4
Journal	Optics Letters
Volume	40
Issue number	9
DOIs	https://doi.org/10.1364/OL.40.002112
Publication status	Published - 1 Jan 2015
MoE publication type	A1 Journal article-refereed

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10.1364/OL.40.002112

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title = "8×10-17 fractional laser frequency instability with a long room-temperature cavity",

abstract = "We present a laser system based on a 48 cm long optical glass resonator. The large size requires a sophisticated thermal control and optimized mounting design. A self-balancing mounting was essential to reliably reach sensitivities to acceleration of below Δν/ν < 2 × 10-10/g in all directions. Furthermore, fiber noise cancellations from a common reference point near the laser diode to the cavity mirror and to additional user points (Sr clock and frequency comb) are implemented. Through comparison with other cavity-stabilized lasers and with a strontium lattice clock, instability of below 1 × 10-16 at averaging times from 1 to 1000 s is revealed.",

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AU - Häfner, Sebastian

AU - Falke, Stephan

AU - Grebing, Christian

AU - Vogt, Stefan

AU - Legero, Thomas

AU - Merimaa, Mikko

AU - Lisdat, Christian

AU - Sterr, Uwe

PY - 2015/1/1

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N2 - We present a laser system based on a 48 cm long optical glass resonator. The large size requires a sophisticated thermal control and optimized mounting design. A self-balancing mounting was essential to reliably reach sensitivities to acceleration of below Δν/ν < 2 × 10-10/g in all directions. Furthermore, fiber noise cancellations from a common reference point near the laser diode to the cavity mirror and to additional user points (Sr clock and frequency comb) are implemented. Through comparison with other cavity-stabilized lasers and with a strontium lattice clock, instability of below 1 × 10-16 at averaging times from 1 to 1000 s is revealed.

AB - We present a laser system based on a 48 cm long optical glass resonator. The large size requires a sophisticated thermal control and optimized mounting design. A self-balancing mounting was essential to reliably reach sensitivities to acceleration of below Δν/ν < 2 × 10-10/g in all directions. Furthermore, fiber noise cancellations from a common reference point near the laser diode to the cavity mirror and to additional user points (Sr clock and frequency comb) are implemented. Through comparison with other cavity-stabilized lasers and with a strontium lattice clock, instability of below 1 × 10-16 at averaging times from 1 to 1000 s is revealed.

U2 - 10.1364/OL.40.002112

DO - 10.1364/OL.40.002112

M3 - Article

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VL - 40

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EP - 2115

JO - Optics Letters

JF - Optics Letters

IS - 9

ER -

8×10-17 fractional laser frequency instability with a long room-temperature cavity

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8×10^-17 fractional laser frequency instability with a long room-temperature cavity