2011
DOI: 10.1016/j.gde.2011.08.004
|View full text |Cite
|
Sign up to set email alerts
|

When multiphoton microscopy sees near infrared

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
10
0

Year Published

2013
2013
2019
2019

Publication Types

Select...
5
2
2

Relationship

1
8

Authors

Journals

citations
Cited by 17 publications
(10 citation statements)
references
References 56 publications
0
10
0
Order By: Relevance
“…Second harmonic light can be generated when two photons with the same frequency interact with non-centrosymmetric structures and are effectively combined to generate a new photon with twice the energy (Mojzisova and Vermot, 2011). This approach allows muscle fibers imaging without any exogenous labeling at high resolution (Plotnikov et al, 2006).…”
Section: Desmin Loss or Aggregation Leads To Muscle Disorganization Amentioning
confidence: 99%
“…Second harmonic light can be generated when two photons with the same frequency interact with non-centrosymmetric structures and are effectively combined to generate a new photon with twice the energy (Mojzisova and Vermot, 2011). This approach allows muscle fibers imaging without any exogenous labeling at high resolution (Plotnikov et al, 2006).…”
Section: Desmin Loss or Aggregation Leads To Muscle Disorganization Amentioning
confidence: 99%
“…The simultaneous absorption of two photons allows, in the case of degenerate TPA, to divide the required energy by a factor of two, i.e., to double the vertical transition wavelength. This permit to notably shift the required incoming photon energy toward the red part of the visible spectrum (i.e., bathochromic shift), eventually allowing to enter in the so-called near-infrared therapeutic window (from 650 to 1350 nm), where the penetration of biological tissues is maximal (Tsai et al, 2001 ; Mojzisova and Vermot, 2011 ).…”
Section: Non-linear Spectroscopymentioning
confidence: 99%
“…This technique is based on parametric down conversions occurring into a birefringent nonlinear crystal. These optical parametric oscillators or amplifiers (OPO or OPA) convert the excitation wavelengths in longer wavelengths [95]. They are pumped by a Ti: Sa source, extending the range of excitation wavelengths available between 0.5 µm up to about 2.5 µm [96][97][98].…”
Section: Laser Technology Usually Implemented On Commercial Multiphotmentioning
confidence: 99%