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Merck KGaA nematic liquid crystals mixture e7
Nematic Liquid Crystals Mixture E7, supplied by Merck KGaA, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
https://www.bioz.com/product/nematic+liquid+crystals+mixture+e7/liquid+crystal+e7/us11353191-361-55-58
Average 90 stars, based on 1 article reviews
nematic liquid crystals mixture e7 - by Bioz Stars, 2026-09
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Article Title: Tunable white illumination
Article Snippet: For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. .. For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..

Article Title: Tunability in sun-light imitating lighting systems
Article Snippet: .. Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based diffuser unit 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..

Adhesive:

Article Title: Tunable white illumination
Article Snippet: For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. .. For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..

Article Title: Tunability in sun-light imitating lighting systems
Article Snippet: .. Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based diffuser unit 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..

Refractive Index:

Article Title: Tunable white illumination
Article Snippet: For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. .. For the PDLC film configuration of NOA65 and E7, FIG. 13 also illustrates the tuning possibilities of the various LC based tuning configurations discussed herein such as the electric field based tuning, the incident angle based tuning, and the polarization based tuning Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based layer structure 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..

Article Title: Tunability in sun-light imitating lighting systems
Article Snippet: .. Specifically, in that configuration, the PDLC film comprises a nematic liquid crystals mixture “E7” produced by Merck KGaA embedded in the Norland Optical Adhesive 65 (known as “NOA65”) produced by Norland optics Inc. With respect to tuning the mismatch of refractive indices (and thus the Rayleigh-like scattering cross-section due to tuning the relative refractive index m), the embodiment of LC based diffuser unit 13 provides for an OFF operation state with the average refractive index n_OFF (i.e. n) applicable to all incidence directions. ..



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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an <t>E7</t> <t>NLC</t> V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .
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Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an E7 NLC V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .

Journal: Sensors (Basel, Switzerland)

Article Title: A Novel Approach for the Creation of Electrically Controlled LC:PDMS Microstructures

doi: 10.3390/s22114037

Figure Lengend Snippet: Results of numerical simulations showing molecular reorientation under the influence of the electric field (with the assumption of the flat electrodes located along the vertical sidewalls—i.e., only the x -component of the electric field and thus the reorientation taking place in the y - x plane is considered). Effective refractive index for y -polarized light beam (see the color bar in the bottom-left corner) is calculated as: n eff,y = n o n e ( n o 2 cos 2 θ + n e 2 sin 2 θ) −1/2 . For an E7 NLC V 1 = 1 V (when taking ε ⊥ = 5.21, ε ‖ = 19.28 as electric permittivity at 1 kHz, and K = 17.1 × 10 −12 N as the elastic constant ). Ordinary and extraordinary refractive indices of E7 NLC are equal to n o = 1.522 and n e = 1.739 @ 589nm, respectively .

Article Snippet: Before testing the samples, the central channel of the structure was filled with an E7 nematic liquid crystal (NLC) mixture (provided by Merck, Darmstadt, Germany).

Techniques: Refractive Index