TY - JOUR

T1 - Terahertz Bessel Beams Formed by Binary and Holographic Axicons

AU - Knyazev, Boris

AU - Osintseva, Natalya

AU - Komlenok, Maxim

AU - Pavelyev, Vladimir

AU - Gerasimov, Vasily

AU - Kameshkov, Oleg

AU - Choporova, Yulia

AU - Tukmakov, Konstantin

N1 - This research was funded in part by the Russian Foundation for Basic Research, grant no. 18-32-20226. Публикация для корректировки.

PY - 2023/6

Y1 - 2023/6

N2 - The characteristics of high-power vortex Bessel beams in the terahertz range (휆=141 μm) obtained with the use of diffractive axicons (DAs) illuminated by a Gaussian beam of the Novosibirsk free-electron laser were studied. Two of the three possible types of DA recently described in our previous paper, namely, binary spiral silicon axicons (BAs), forming beams with a topological charge l equal to 0–4 and 9, and a diamond “holographic” axicon (HA), forming a beam with 푙=9, were used in the experiments. These axicons formed beams whose cross sections in the region of inner Bessel rings were close to those of ideal Bessel beams, but their intensities varied in azimuth with a frequency of l and 2푙 for the BAs and HA, respectively. However, in the case of the BAs, the beams had a pronounced helical structure at the periphery, whereas for the HA, the beam was axisymmetric. By focusing these beams with a lens, we studied the structure of the so-called “perfect” beams (PBs). While an ideal Bessel beam exhibits a PB as a thin ring, in the case of the BAs, we observed a broadened ring structure consisting of 2푙 short spirals, and for the HA, we observed a narrow ring with 2푙 maxima in azimuth. A comparison of the numerical calculations and experiments showed that the observed azimuthal intensity variations can be attributed to inaccuracies in the preparation of the axicon relief and/or discrepancies between the calculated and actual wavelengths, within a few percent. The results of this work enable the establishment of quality requirements for axicon manufacture and the appropriate selection of the axicon type in accordance with the requirements for the beam.

AB - The characteristics of high-power vortex Bessel beams in the terahertz range (휆=141 μm) obtained with the use of diffractive axicons (DAs) illuminated by a Gaussian beam of the Novosibirsk free-electron laser were studied. Two of the three possible types of DA recently described in our previous paper, namely, binary spiral silicon axicons (BAs), forming beams with a topological charge l equal to 0–4 and 9, and a diamond “holographic” axicon (HA), forming a beam with 푙=9, were used in the experiments. These axicons formed beams whose cross sections in the region of inner Bessel rings were close to those of ideal Bessel beams, but their intensities varied in azimuth with a frequency of l and 2푙 for the BAs and HA, respectively. However, in the case of the BAs, the beams had a pronounced helical structure at the periphery, whereas for the HA, the beam was axisymmetric. By focusing these beams with a lens, we studied the structure of the so-called “perfect” beams (PBs). While an ideal Bessel beam exhibits a PB as a thin ring, in the case of the BAs, we observed a broadened ring structure consisting of 2푙 short spirals, and for the HA, we observed a narrow ring with 2푙 maxima in azimuth. A comparison of the numerical calculations and experiments showed that the observed azimuthal intensity variations can be attributed to inaccuracies in the preparation of the axicon relief and/or discrepancies between the calculated and actual wavelengths, within a few percent. The results of this work enable the establishment of quality requirements for axicon manufacture and the appropriate selection of the axicon type in accordance with the requirements for the beam.

KW - Bessel beams

KW - diffractive axicons

KW - free-electron laser

KW - terahertz radiation

UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-85163849216&origin=inward&txGid=d60260562f5e1badfafb774370182fd2

UR - https://www.mendeley.com/catalogue/03435e29-6af9-35c7-92ed-dabeeee4ed6c/

U2 - 10.3390/photonics10060700

DO - 10.3390/photonics10060700

M3 - Article

VL - 10

JO - Photonics

JF - Photonics

SN - 2304-6732

IS - 6

M1 - 700

ER -