2013
DOI: 10.1007/s00340-013-5678-9
|View full text |Cite
|
Sign up to set email alerts
|

Second harmonic generation by micropowders: a revision of the Kurtz–Perry method and its practical application

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
58
0

Year Published

2015
2015
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 40 publications
(60 citation statements)
references
References 43 publications
2
58
0
Order By: Relevance
“…At first, the THG signal may be directly generated by the surface of the sample within the surface coherence length L c,s =π/(k(3ω)+3k(ω)), where k(3ω) and k(ω) are the wave-vectors at the fundamental and third harmonic frequencies, respectively. Since the theory for THG in the limit of weak pump depletion is the same as for SHG, the irradiance of this THG signal writes 3 ∝ where 3 is the effective susceptibility of our sample and I(ω) is the light irradiance at the fundamental frequency ω [8][9][10]. Note that, due to the very small value of L c,s (<0.1 µm), the absorption of the THG signal within this length interval can be neglected.…”
Section: Resultsmentioning
confidence: 99%
“…At first, the THG signal may be directly generated by the surface of the sample within the surface coherence length L c,s =π/(k(3ω)+3k(ω)), where k(3ω) and k(ω) are the wave-vectors at the fundamental and third harmonic frequencies, respectively. Since the theory for THG in the limit of weak pump depletion is the same as for SHG, the irradiance of this THG signal writes 3 ∝ where 3 is the effective susceptibility of our sample and I(ω) is the light irradiance at the fundamental frequency ω [8][9][10]. Note that, due to the very small value of L c,s (<0.1 µm), the absorption of the THG signal within this length interval can be neglected.…”
Section: Resultsmentioning
confidence: 99%
“…The maximal SHG signal is found for particle size r~ l C and odd multiples of l C . This model does not take into account many other parameters, e.g., the scattering of the crystalline particles of the sample, and has recently been revisited by Aramburu et al [28] from a theoretical point of view, but also from an experimental viewpoint as, e.g., sample preparation and detection geometry [29,30]. 2).…”
Section: Phase-matching Properties In a Randommentioning
confidence: 99%
“…Measurements in both setups are performed in reflection geometry, i.e., the backward SHG light is collected, which is the most commonly encountered case [28]. Actually, the SHG light is scattered in all directions and only one part is detected.…”
Section: Experimental Setup For P-shg and Tr-shgmentioning
confidence: 99%
See 1 more Smart Citation
“…Compared to this version of the material, while comprehensively studied [3] and well exploited technologically [4][5][6], powders are tacitly considered easier and far less expensive to synthesize. LN powders (LNPws) have served in the past only as survey materials, for example, in the prediction of the nonlinear second order optical capabilities of unavailable single crystals by applying the Kurtz-Perry method in the powdered version [7,8]. Nevertheless, recent developments in LNPws are certainly attracting the attention of scientists and engineers who seek to exploit their potential use in a wide range of applications that span from the construction industry to nonlinear optics.…”
Section: Introductionmentioning
confidence: 99%