J W Nicholson

Summary

Publications

  1. doi request reprint Raman fiber laser with 81 W output power at 1480 nm
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Lett 35:3069-71. 2010
  2. doi request reprint Scaling the effective area of higher-order-mode erbium-doped fiber amplifiers
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Express 20:24575-84. 2012
  3. doi request reprint Measuring higher-order modes in a low-loss, hollow-core, photonic-bandgap fiber
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Express 20:20494-505. 2012
  4. ncbi request reprint Spatially and spectrally resolved imaging of modal content in large-mode-area fibers
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Rd, Suite 105, Somerset, NJ 08873, USA
    Opt Express 16:7233-43. 2008
  5. doi request reprint A higher-order-mode erbium-doped-fiber amplifier
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, NJ 08873, USA
    Opt Express 18:17651-7. 2010
  6. ncbi request reprint Simultaneous direct amplification and compression of picosecond pulses to 65-kW peak power without pulse break-up in erbium fiber
    J C Jasapara
    OFS Laboratories, 19 Schoolhouse Rd, Somerset, NJ 08873, USA
    Opt Express 15:17494-501. 2007
  7. ncbi request reprint Diffraction limited amplification of picosecond pulses in 1170 microm2 effective area erbium fiber
    J C Jasapara
    OFS Laboratories, Somerset, NJ 08873, USA
    Opt Express 16:18869-74. 2008

Detail Information

Publications7

  1. doi request reprint Raman fiber laser with 81 W output power at 1480 nm
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Lett 35:3069-71. 2010
    ..A cascaded Raman fiber with a long-wavelength fundamental mode cutoff enables efficient multiple Stokes scattering from 1117 to 1480 nm while preventing further unwanted scattering to 1590 nm...
  2. doi request reprint Scaling the effective area of higher-order-mode erbium-doped fiber amplifiers
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Express 20:24575-84. 2012
    ..CW and pulsed amplifier experiments are reported. Nanosecond pulses are amplified to 0.5 mJ pulse energy with 0.5 MW peak power...
  3. doi request reprint Measuring higher-order modes in a low-loss, hollow-core, photonic-bandgap fiber
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, New Jersey 08873, USA
    Opt Express 20:20494-505. 2012
    ..This measurement is used to illustrate the HOM content as function of coil diameter...
  4. ncbi request reprint Spatially and spectrally resolved imaging of modal content in large-mode-area fibers
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Rd, Suite 105, Somerset, NJ 08873, USA
    Opt Express 16:7233-43. 2008
    ..We refer to the measurement as Spatially and Spectrally resolved imaging of mode content in fibers, or more simply as S(2) imaging...
  5. doi request reprint A higher-order-mode erbium-doped-fiber amplifier
    J W Nicholson
    OFS Laboratories, 19 Schoolhouse Road, Suite 105, Somerset, NJ 08873, USA
    Opt Express 18:17651-7. 2010
    ..A maximum output power of 5.8 W at 1564 nm with more than 20 dB of gain in a 2.68 m long amplifier was obtained. The mode profile was undistorted at the highest output power...
  6. ncbi request reprint Simultaneous direct amplification and compression of picosecond pulses to 65-kW peak power without pulse break-up in erbium fiber
    J C Jasapara
    OFS Laboratories, 19 Schoolhouse Rd, Somerset, NJ 08873, USA
    Opt Express 15:17494-501. 2007
    ....
  7. ncbi request reprint Diffraction limited amplification of picosecond pulses in 1170 microm2 effective area erbium fiber
    J C Jasapara
    OFS Laboratories, Somerset, NJ 08873, USA
    Opt Express 16:18869-74. 2008
    ..A small increase in input pulse energy results in a temporal collapse of the pulse center to 58 fs duration, with peak powers approaching 200 kW...