JPWO2020196317A5 - - Google Patents
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- JPWO2020196317A5 JPWO2020196317A5 JP2020534999A JP2020534999A JPWO2020196317A5 JP WO2020196317 A5 JPWO2020196317 A5 JP WO2020196317A5 JP 2020534999 A JP2020534999 A JP 2020534999A JP 2020534999 A JP2020534999 A JP 2020534999A JP WO2020196317 A5 JPWO2020196317 A5 JP WO2020196317A5
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- film
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以下、本発明について実施例を挙げて説明するが、本発明は必ずしもこれらに限定されるものではない。なお、実施例13、実施例14は、現在は参考例1、参考例2である。 EXAMPLES The present invention will be described below with reference to Examples, but the present invention is not necessarily limited to these. Incidentally, Examples 13 and 14 are Reference Examples 1 and 2 at present.
Claims (19)
(1)前記光源から出射する光線の透過率が、当該光線の最も強い強度の波長において70%以上100%以下であること。
(2)下記(I)式を満足する整数nが存在すること。
(I)A×n-150 ≦ Re ≦ A×n+150
ここで、Aは前記光源から出射する光線において最も強い強度を示す波長(nm)であり、
Reは前記フィルムを平行ニコル回転法を用いて入射角0°での波長587.8nmで測定したときの面内位相差(nm)である。
(3)前記フィルムの面内位相差が400nm以上である。
(4)前記フィルムの主配向軸方向および主配向軸と直交する方向の25℃における破断点伸度がいずれも30%以上300%以下である。 An authentication device having a light source, a polarizer, a film, and a photosensitivity sensor, wherein the film is disposed between the polarizer and an authentication object, and the following (1) , (2), (3) and ( 4) An authentication device characterized by satisfying 4) .
(1) The transmittance of light emitted from the light source is 70% or more and 100% or less at the wavelength of the light with the highest intensity.
(2) There exists an integer n that satisfies the following formula (I).
(I) A×n−150≦Re≦A×n+150
Here, A is the wavelength (nm) at which the light emitted from the light source exhibits the strongest intensity,
Re is the in-plane retardation (nm) when the film is measured at a wavelength of 587.8 nm at an incident angle of 0° using the parallel Nicols rotation method.
(3) The in-plane retardation of the film is 400 nm or more.
(4) The elongation at break at 25°C in both the direction of the main orientation axis and the direction perpendicular to the main orientation axis of the film is 30% or more and 300% or less.
(II)B×m-150 ≦ Re ≦ B×m+150
ここで、Bは前記光源から出射する光線において2番目に強い強度を示す波長(nm)であり、
Reは前記フィルムを平行ニコル回転法を用いて入射角0°での波長587.8nmで測定したときの面内位相差(nm)である。 2. The authentication device according to claim 1, wherein there is an integer m that satisfies the formula (I) and the formula (II) below.
(II) B×m−150≦Re≦B×m+150
Here, B is the wavelength (nm) showing the second strongest intensity in the light emitted from the light source,
Re is the in-plane retardation (nm) when the film is measured at a wavelength of 587.8 nm at an incident angle of 0° using the parallel Nicols rotation method.
(III) PT(45) ≧ 0.65
(IV)1 ≧ PT(45)/ PT(0)≧ 0.6
ここで、PT(45)とPT(0)は下記のとおりで求められる。
(1)偏光子を2枚にカットし、2枚の偏光子の面が50Wタングステンランプを光源とした分光光度計の光軸に垂直になるように、かつ2枚の偏光子の透過軸同士が平行になるように配置し、光源消灯状態と光源点灯状態でのバックグラウンド測定を行う。光源消灯状態で測定された透過光量をPT(D)、光源点灯状態で測定された透過光量をPT(L)とする。
(2)2枚の偏光子の間に前記フィルムをフィルムの面が分光光度計の光軸に垂直になるように配置する。
(3)前記フィルムのみを分光光度計の光軸に垂直な面内で回転させつつ、前記光源から出射する光線の最も強い強度を持つ波長における透過光量の測定を行う。2枚の偏光子の透過軸と前記フィルムの主配向軸のなす角が0°のときの透過光量をPT’(0)、45°のときの透過光量をPT’(45)とする。
(4)下記式よりPT(0)、PT(45)を得る。
PT(0)=(PT’(0)- PT(D))/(PT(L)- PT(D))
PT(45)=(PT’(45)- PT(D))/(PT(L)- PT(D))。 3. The authentication device according to claim 1, wherein the film satisfies the following formulas (III) and (IV).
(III) PT(45) ≥ 0.65
(IV) 1≧PT(45)/PT(0)≧0.6
Here, PT(45) and PT(0) are obtained as follows.
(1) Cut the polarizer into two pieces so that the surfaces of the two polarizers are perpendicular to the optical axis of a spectrophotometer using a 50 W tungsten lamp as a light source, and the transmission axes of the two polarizers are aligned. are arranged parallel to each other, and the background measurement is performed with the light source turned off and the light source turned on. Let PT(D) be the amount of transmitted light measured with the light source off, and PT(L) be the amount of transmitted light measured with the light source on.
(2) The film is placed between two polarizers so that the plane of the film is perpendicular to the optical axis of the spectrophotometer.
(3) While rotating only the film in a plane perpendicular to the optical axis of the spectrophotometer, measure the amount of transmitted light at the wavelength with the highest intensity of light emitted from the light source. Let PT'(0) be the amount of transmitted light when the angle formed by the transmission axes of the two polarizers and the main orientation axis of the film is 0°, and let PT'(45) be the amount of transmitted light when the angle is 45°.
(4) PT(0) and PT(45) are obtained from the following equations.
PT(0)=(PT'(0)-PT(D))/(PT(L)-PT(D))
PT(45)=(PT'(45)-PT(D))/(PT(L)-PT(D)).
(V)A×n-120 ≦ Re ≦ A×n+120、 かつ、415 ≦ A ≦ 495。 5. The authentication device according to any one of claims 1 to 4, wherein there is an integer n that satisfies the following formula (V).
(V) A×n−120≦Re≦A×n+120, and 415≦A≦495.
(VI)A×n-100 ≦ Re ≦ A×n+100、かつ、495 ≦ A ≦ 570。 5. The authentication device according to any one of claims 1 to 4, wherein there is an integer n that satisfies the following formula (VI).
(VI) A×n−100≦Re≦A×n+100 and 495≦A≦570.
(VII)A×n-120 ≦ Re ≦ A×n+120、かつ、570 ≦ A ≦ 800。 5. The authentication device according to any one of claims 1 to 4, wherein there is an integer n that satisfies the following formula (VII).
(VII) A×n−120≦Re≦A×n+120 and 570≦A≦800.
(VIII)A×n-150 ≦ Re ≦ A×n+150、かつ、800 ≦ A ≦ 1600。 5. The authentication device according to any one of claims 1 to 4, wherein there is an integer n that satisfies the following formula (VIII).
(VIII) A×n−150≦Re≦A×n+150 and 800≦A≦1600.
(1)前記フィルムが、前記光源から出射する光線の透過率が、当該光線の最も強い強度の波長において70%以上100%以下であること。
(2)下記(I)式を満足する整数nが存在すること。
(I)A×n-150 ≦ Re ≦ A×n+150
ここで、Aは前記光源から出射する光線において最も強い強度を示す波長(nm)であり、
Reは前記フィルムを平行ニコル回転法を用いて入射角0°での波長587.8nmで測定したときの面内位相差(nm)である。
(3)前記フィルムの面内位相差が400nm以上である。
(4)前記フィルムの主配向軸方向および主配向軸と直交する方向の25℃における破断点伸度がいずれも30%以上300%以下である。 A film used in an authentication device having a light source, a polarizer, a film, and a photosensitivity sensor, which satisfies the following (1) , (2), (3) and (4) .
(1) The film has a transmittance of light emitted from the light source of 70% or more and 100% or less at the wavelength with the highest intensity of the light.
(2) There exists an integer n that satisfies the following formula (I).
(I) A×n−150≦Re≦A×n+150
Here, A is the wavelength (nm) at which the light emitted from the light source exhibits the strongest intensity,
Re is the in-plane retardation (nm) when the film is measured at a wavelength of 587.8 nm at an incident angle of 0° using the parallel Nicols rotation method.
(3) The in-plane retardation of the film is 400 nm or more.
(4) The elongation at break at 25°C in both the direction of the main orientation axis and the direction perpendicular to the main orientation axis of the film is 30% or more and 300% or less.
(III) PT(45) ≧ 0.65
(IV)1 ≧ PT(45)/ PT(0)≧ 0.6
ここで、PT(45)とPT(0)は下記のとおりで求められる。
(1)偏光子を2枚にカットし、2枚の偏光子の面が50Wタングステンランプを光源とした分光光度計の光軸に垂直になるように、かつ2枚の偏光子の透過軸同士が平行になるように配置し、バックグラウンド測定を行う。光源消灯状態で測定された透過光量をPT(D)、光源点灯状態で測定された透過光量をPT(L)とする。
(2)2枚の偏光子の間に前記フィルムをフィルムの面が分光光度計の光軸に垂直になるように配置する。
(3)前記フィルムのみを分光光度計の光軸に垂直な面内で回転させつつ、前記光源から出射する光線において最も強い強度を示す波長における透過光量の測定を行う。2枚の偏光子の透過軸と前記フィルムの主配向軸のなす角が0°のときの透過光量をPT’(0)、45°のときの透過光量をPT’(45)とする。
(4)下記式よりPT(0)、PT(45)を得る。
PT(0)=(PT’(0)- PT(D))/(PT(L)- PT(D))
PT(45)=(PT’(45)- PT(D))/(PT(L)- PT(D))。 19. The film according to claim 18 , wherein said film satisfies formulas (III) and (IV) below.
(III) PT(45) ≥ 0.65
(IV) 1≧PT(45)/PT(0)≧0.6
Here, PT(45) and PT(0) are obtained as follows.
(1) Cut the polarizer into two pieces so that the surfaces of the two polarizers are perpendicular to the optical axis of a spectrophotometer using a 50 W tungsten lamp as a light source, and the transmission axes of the two polarizers are aligned. background measurement. Let PT(D) be the amount of transmitted light measured with the light source off, and PT(L) be the amount of transmitted light measured with the light source on.
(2) The film is placed between two polarizers so that the plane of the film is perpendicular to the optical axis of the spectrophotometer.
(3) While rotating only the film in a plane perpendicular to the optical axis of the spectrophotometer, measure the amount of transmitted light at the wavelength at which the light emitted from the light source exhibits the highest intensity. Let PT'(0) be the amount of transmitted light when the angle formed by the transmission axes of the two polarizers and the main orientation axis of the film is 0°, and let PT'(45) be the amount of transmitted light when the angle is 45°.
(4) PT(0) and PT(45) are obtained from the following equations.
PT(0)=(PT'(0)-PT(D))/(PT(L)-PT(D))
PT(45)=(PT'(45)-PT(D))/(PT(L)-PT(D)).
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2019063197 | 2019-03-28 | ||
PCT/JP2020/012450 WO2020196317A1 (en) | 2019-03-28 | 2020-03-19 | Authentication device and film |
Publications (2)
Publication Number | Publication Date |
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JPWO2020196317A1 JPWO2020196317A1 (en) | 2020-10-01 |
JPWO2020196317A5 true JPWO2020196317A5 (en) | 2023-03-14 |
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JP2020534999A Pending JPWO2020196317A1 (en) | 2019-03-28 | 2020-03-19 |
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JP (1) | JPWO2020196317A1 (en) |
KR (1) | KR20210143754A (en) |
CN (1) | CN113574427B (en) |
WO (1) | WO2020196317A1 (en) |
Family Cites Families (9)
Publication number | Priority date | Publication date | Assignee | Title |
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JP4644916B2 (en) * | 2000-07-25 | 2011-03-09 | 東レ株式会社 | Polyester film for polarizing film lamination |
JP5609086B2 (en) * | 2009-12-04 | 2014-10-22 | 東レ株式会社 | Polarized reflector |
CN102322880B (en) * | 2011-08-18 | 2013-06-05 | 天津大学 | Polarization sensitive distributive optical frequency domain reflection disturbance sensor and demodulation method |
WO2015156199A1 (en) * | 2014-04-09 | 2015-10-15 | 東レ株式会社 | Polarizer-protecting polyester film, and polarization plate obtained using same |
WO2017126153A1 (en) | 2016-01-22 | 2017-07-27 | コニカミノルタ株式会社 | Optical fingerprint authentication device |
JP2018189725A (en) * | 2017-04-28 | 2018-11-29 | Jsr株式会社 | Optical filter and image capturing device using the same |
JP2018194620A (en) * | 2017-05-15 | 2018-12-06 | Jsr株式会社 | Optical filter |
EP3851884A4 (en) * | 2018-09-12 | 2022-06-08 | Toray Industries, Inc. | Laminate film |
CN112740304A (en) * | 2018-09-28 | 2021-04-30 | 东洋纺株式会社 | Image display device with fingerprint verification sensor |
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2020
- 2020-03-19 WO PCT/JP2020/012450 patent/WO2020196317A1/en active Application Filing
- 2020-03-19 JP JP2020534999A patent/JPWO2020196317A1/ja active Pending
- 2020-03-19 CN CN202080021395.7A patent/CN113574427B/en active Active
- 2020-03-19 KR KR1020217029171A patent/KR20210143754A/en active Search and Examination
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