5 research outputs found
Chiral discrimination in optical trapping and manipulation
When circularly polarized light interacts with chiral molecules or nanoscale particles powerful symmetry principles determine the possibility of achieving chiral discrimination, and the detailed form of electrodynamic mechanisms dictate the types of interaction that can be involved. The optical trapping of molecules and nanoscale particles can be described in terms of a forward-Rayleigh scattering mechanism, with trapping forces being dependent on the positioning within the commonly non-uniform intensity beam profile. In such a scheme, nanoparticles are commonly attracted to local potential energy minima, ordinarily towards the centre of the beam. For achiral particles the pertinent material response property usually entails an electronic polarizability involving transition electric dipole moments. However, in the case of chiral molecules, additional effects arise through the engagement of magnetic counterpart transition dipoles. It emerges that, when circularly polarized light is used for the trapping, a discriminatory response can be identified between left- and right-handed polarizations. Developing a quantum framework to accurately describe this phenomenon, with a tensor formulation to correctly represent the relevant molecular properties, the theory leads to exact analytical expressions for the associated energy landscape contributions. Specific results are identified for liquids and solutions, both for isotropic media and also where partial alignment arises due to a static electric field. The paper concludes with a pragmatic analysis of the scope for achieving enantiomer separation by such methods
ΠΠΎΠ²ΡΡΠ΅Π½ΠΈΠ΅ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΠΎΠ³ΠΎ ΡΠ΅ΡΠΌΠΎΡΠ°ΡΠΊΠ°Π»ΡΠ²Π°Π½ΠΈΡ ΡΠΈΠ»ΠΈΠΊΠ°ΡΠ½ΡΡ ΡΡΠ΅ΠΊΠΎΠ» Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΠΎΠ΄Π° ΡΠΎΡΠΎΡΠΏΡΡΠ³ΠΎΡΡΠΈ
A method for monitoring the development of a separating crack in the process of laser-controlled thermal splitting of silicate glasses is proposed. This method is based on the polarization-optical method (photoelasticity
method). The method was developed on the basis of numerical modeling and experimental studies of the process
using a polarized light source and a video camera with an analyzer. During the cutting process, a source of polarized light creates a stream, which, passing through silicate glass, enters a video camera with an analyzer. Analysis
of the parameters of polarized light in the area of material processing allows us to drawa conclusion about the stable development or absence of the formation of a separating microcrack. Based on the information obtained, it is
necessary to dynamically make corrections to the technological parameters of the laser thermal splitting process for
separating silicate glasses to maintain the value of thermoelastic stresses necessary for the formation of a microcrack, or transmit a command to interrupt the process.ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½ ΠΌΠ΅ΡΠΎΠ΄ ΠΊΠΎΠ½ΡΡΠΎΠ»Ρ ΡΠ°Π·Π²ΠΈΡΠΈΡ ΡΠ°Π·Π΄Π΅Π»ΡΡΡΠ΅ΠΉ ΡΡΠ΅ΡΠΈΠ½Ρ Π² ΠΏΡΠΎΡΠ΅ΡΡΠ΅ Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠΏΡΠ°Π²Π»ΡΠ΅ΠΌΠΎΠ³ΠΎ
ΡΠ΅ΡΠΌΠΎΡΠ°ΡΠΊΠ°Π»ΡΠ²Π°Π½ΠΈΡ ΡΠΈΠ»ΠΈΠΊΠ°ΡΠ½ΡΡ
ΡΡΠ΅ΠΊΠΎΠ», Π² ΠΎΡΠ½ΠΎΠ²Π΅ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ Π»Π΅ΠΆΠΈΡ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΎΠ½Π½ΠΎ-ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠΉ ΠΌΠ΅ΡΠΎΠ΄ (ΠΌΠ΅ΡΠΎΠ΄ ΡΠΎΡΠΎΡΠΏΡΡΠ³ΠΎΡΡΠΈ). ΠΠ΅ΡΠΎΠ΄ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½ Π½Π° Π±Π°Π·Π΅ ΡΠΈΡΠ»Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΡΠΎΡΠ΅ΡΡΠ° Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ²Π΅ΡΠ° ΠΈ Π²ΠΈΠ΄Π΅ΠΎΠΊΠ°ΠΌΠ΅ΡΡ Ρ Π°Π½Π°Π»ΠΈΠ·Π°ΡΠΎΡΠΎΠΌ.
ΠΠΎ Π²ΡΠ΅ΠΌΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΡΠ΅Π·ΠΊΠΈ ΠΈΡΡΠΎΡΠ½ΠΈΠΊ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ²Π΅ΡΠ° ΡΠΎΠ·Π΄Π°Π΅Ρ ΠΏΠΎΡΠΎΠΊ, ΠΊΠΎΡΠΎΡΡΠΉ, ΠΏΡΠΎΡ
ΠΎΠ΄Ρ ΡΠ΅ΡΠ΅Π· ΡΠΈΠ»ΠΈΠΊΠ°ΡΠ½ΠΎΠ΅ ΡΡΠ΅ΠΊΠ»ΠΎ, ΠΏΠΎΠΏΠ°Π΄Π°Π΅Ρ Π² Π²ΠΈΠ΄Π΅ΠΎΠΊΠ°ΠΌΠ΅ΡΡ Ρ Π°Π½Π°Π»ΠΈΠ·Π°ΡΠΎΡΠΎΠΌ. ΠΠ½Π°Π»ΠΈΠ· ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠ²Π΅ΡΠ° Π² ΠΎΠ±Π»Π°ΡΡΠΈ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΡΠ΄Π΅Π»Π°ΡΡ Π²ΡΠ²ΠΎΠ΄ ΠΎΠ± ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΠΌ ΡΠ°Π·Π²ΠΈΡΠΈΠΈ ΠΈΠ»ΠΈ ΠΎΡΡΡΡΡΡΠ²ΠΈΠΈ ΠΎΠ±ΡΠ°Π·ΠΎΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π΄Π΅Π»ΡΡΡΠ΅ΠΉ ΠΌΠΈΠΊΡΠΎΡΡΠ΅ΡΠΈΠ½Ρ. ΠΠΎ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΠΎΠΉ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΈ Π²Π½ΠΎΡΠΈΡΡ
ΠΊΠΎΡΡΠ΅ΠΊΡΠΈΡ Π² ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° Π»Π°Π·Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΡΠΌΠΎΡΠ°ΡΠΊΠ°Π»ΡΠ²Π°Π½ΠΈΡ ΡΠ°Π·Π΄Π΅Π»Π΅Π½ΠΈΡ ΡΠΈΠ»ΠΈΠΊΠ°ΡΠ½ΡΡ
ΡΡΠ΅ΠΊΠΎΠ» Π΄Π»Ρ ΠΏΠΎΠ΄Π΄Π΅ΡΠΆΠ°Π½ΠΈΡ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΡΠ΅ΡΠΌΠΎΡΠΏΡΡΠ³ΠΈΡ
Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ, Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΡΡ
Π΄Π»Ρ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΌΠΈΠΊΡΠΎΡΡΠ΅ΡΠΈΠ½Ρ, Π»ΠΈΠ±ΠΎ ΠΏΠ΅ΡΠ΅Π΄Π°Π²Π°ΡΡ ΠΊΠΎΠΌΠ°Π½Π΄Ρ ΠΏΡΠ΅ΡΡΠ²Π°Π½ΠΈΡ ΠΏΡΠΎΡΠ΅ΡΡΠ°