JP2014197536A5 - - Google Patents
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- JP2014197536A5 JP2014197536A5 JP2014041321A JP2014041321A JP2014197536A5 JP 2014197536 A5 JP2014197536 A5 JP 2014197536A5 JP 2014041321 A JP2014041321 A JP 2014041321A JP 2014041321 A JP2014041321 A JP 2014041321A JP 2014197536 A5 JP2014197536 A5 JP 2014197536A5
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- 230000003595 spectral Effects 0.000 claims 41
- 235000010956 sodium stearoyl-2-lactylate Nutrition 0.000 claims 25
- 241001106462 Ulmus Species 0.000 claims 24
- 238000005286 illumination Methods 0.000 claims 16
- OAICVXFJPJFONN-UHFFFAOYSA-N phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 claims 15
- 230000002596 correlated Effects 0.000 claims 11
- 238000000295 emission spectrum Methods 0.000 claims 10
- 239000004065 semiconductor Substances 0.000 claims 10
- 239000011575 calcium Substances 0.000 claims 9
- 229910052788 barium Inorganic materials 0.000 claims 8
- 229910052712 strontium Inorganic materials 0.000 claims 8
- 229910052791 calcium Inorganic materials 0.000 claims 7
- 230000005457 Black-body radiation Effects 0.000 claims 4
- 230000001443 photoexcitation Effects 0.000 claims 3
- 102100001764 ALS2 Human genes 0.000 claims 2
- 101700045037 ALS2 Proteins 0.000 claims 2
- 229910052749 magnesium Inorganic materials 0.000 claims 2
- CPLXHLVBOLITMK-UHFFFAOYSA-N magnesium oxide Chemical compound [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 claims 2
- 239000011701 zinc Substances 0.000 claims 2
- 230000035839 C max Effects 0.000 claims 1
- 229910052691 Erbium Inorganic materials 0.000 claims 1
- 229910052693 Europium Inorganic materials 0.000 claims 1
- 229910052688 Gadolinium Inorganic materials 0.000 claims 1
- 229910005793 GeO 2 Inorganic materials 0.000 claims 1
- 229910052765 Lutetium Inorganic materials 0.000 claims 1
- 229910020068 MgAl Inorganic materials 0.000 claims 1
- 229910017639 MgSi Inorganic materials 0.000 claims 1
- 229910052772 Samarium Inorganic materials 0.000 claims 1
- 229910004018 SiF Inorganic materials 0.000 claims 1
- 229910004283 SiO 4 Inorganic materials 0.000 claims 1
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium(0) Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 claims 1
- OYPRJOBELJOOCE-UHFFFAOYSA-N calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 claims 1
- 229910052748 manganese Inorganic materials 0.000 claims 1
- 239000000203 mixture Substances 0.000 claims 1
- 230000003287 optical Effects 0.000 claims 1
- 229910052761 rare earth metal Inorganic materials 0.000 claims 1
- 229910052706 scandium Inorganic materials 0.000 claims 1
- CIOAGBVUUVVLOB-UHFFFAOYSA-N strontium Chemical compound [Sr] CIOAGBVUUVVLOB-UHFFFAOYSA-N 0.000 claims 1
- 229910052727 yttrium Inorganic materials 0.000 claims 1
- HCHKCACWOHOZIP-UHFFFAOYSA-N zinc Chemical compound [Zn] HCHKCACWOHOZIP-UHFFFAOYSA-N 0.000 claims 1
- 229910052725 zinc Inorganic materials 0.000 claims 1
Claims (38)
波長をλ(nm)とし、
当該発光要素から主たる放射方向に出射される光の分光分布をΦelm(λ)、当該発光装置から主たる放射方向に出射される光の分光分布をφSSL(λ)とし、
Φelm(λ)は下記条件1と条件3´の少なくともいずれか一方を満たさず、φSSL(λ)は下記条件1と条件3´をともに満たすことを特徴とする発光装置。
条件1:
対象となる光の分光分布におけるANSI C78.377で定義される黒体放射軌跡からの距離Duvが、−0.0350 ≦ Duv < 0となる光を含む。
条件3´:
対象となる光の分光分布による照明を数学的に仮定した場合の#01から#15の下記15種類の修正マンセル色票のCIE 1976 L * a * b * 色空間におけるa * 値、b *
値をそれぞれa * n 、b * n (ただしnは1から15の自然数)とし、
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L *
a * b * 色空間におけるa * 値、b * 値をそれぞれa * nref 、b * nref (ただしnは1から15の自然数)とした場合に、飽和度差ΔC n が
−3.8 ≦ ΔC n ≦ 18.6 (nは1から15の自然数)
を満たす。
ただし、ΔC n =√{(a * n ) 2 +(b * n ) 2 }−√{(a * nref ) 2 +(b * nr
ef ) 2 }とする。
15種類の修正マンセル色票
#01 7.5 P 4 /10
#02 10 PB 4 /10
#03 5 PB 4 /12
#04 7.5 B 5 /10
#05 10 BG 6 / 8
#06 2.5 BG 6 /10
#07 2.5 G 6 /12
#08 7.5 GY 7 /10
#09 2.5 GY 8 /10
#10 5 Y 8.5/12
#11 10 YR 7 /12
#12 5 YR 7 /12
#13 10 R 6 /12
#14 5 R 4 /14
#15 7.5 RP 4 /12 A light-emitting device having a light-emitting element and a control element in which a semiconductor light-emitting element is embedded,
Let the wavelength be λ (nm),
The spectral distribution of the light emitted from the light emitting element in the main radiation direction is Φ elm (λ), the spectral distribution of the light emitted from the light emitting device in the main radiation direction is φ SSL (λ),
Φ elm (λ) does not satisfy at least one of the following conditions 1 and 3 ′, and φ SSL (λ) satisfies both of the following conditions 1 and 3 ′ .
Condition 1:
Including the light in which the distance D uv from the black body radiation locus defined in ANSI C78.377 in the spectral distribution of the target light is −0.0350 ≦ D uv <0 .
Condition 3 ′:
CIE 1976 L * a * b * a * value in color space , b * of the following 15 types of modified Munsell color charts from # 01 to # 15 when the illumination by the spectral distribution of the target light is mathematically assumed
The values are a * n and b * n (where n is a natural number from 1 to 15),
CIE 1976 L * of the 15 types of modified Munsell color charts when mathematically assuming illumination with reference light selected according to the correlated color temperature T (K) of light emitted in the radiation direction
a * b * a * values in a color space, b * values, respectively a * nref, when the b * nref (where n is a natural number of 1 to 15), the saturation difference [Delta] C n
−3.8 ≦ ΔC n ≦ 18.6 (n is a natural number from 1 to 15)
Meet.
However, ΔC n = √ {(a * n ) 2 + (b * n ) 2 } −√ {(a * nref ) 2 + (b * nr
ef ) 2 }.
15 kinds of modified Munsell color chart
# 01 7.5 P 4/10
# 02 10 PB 4/10
# 03 5 PB 4/12
# 04 7.5 B 5/10
# 05 10 BG 6/8
# 06 2.5 BG 6/10
# 07 2.5 G 6/12
# 08 7.5 GY 7/10
# 09 2.5 GY 8/10
# 10 5 Y 8.5 / 12
# 11 10 YR 7/12
# 12 5 YR 7/12
# 13 10 R 6/12
# 14 5 R 4/14
# 15 7.5 RP 4/12
条件3´´:
飽和度差の最大値をΔCmax、飽和度差の最小値をΔCminとした場合に、飽和度差の最大値と、飽和度差の最小値との間の差|ΔCmax−ΔCmin|が
2.8 ≦ |ΔCmax−ΔCmin| ≦ 19.6
を満たす。
条件4:
対象となる光の分光分布による照明を数学的に仮定した場合の上記15種類の修正マンセル色票のCIE 1976 L*a*b*色空間における色相角をθn(度)(ただしn
は1から15の自然数)とし、
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L*
a*b*色空間における色相角をθnref(度)(ただしnは1から15の自然数)とした場合に、色相角差の絶対値|Δhn|が
0 ≦ |Δhn| ≦ 9.0(度)(nは1から15の自然数)
を満たす。
ただし、Δhn=θn−θnrefとする。 A light emitting device according to claim 1, Φ elm (λ) does not satisfy at least one of the following conditions 3'' and condition 4, the phi SSL (lambda) is the following condition 3'' and condition 4 A light emitting device characterized by satisfying both.
Condition 3 ″ :
[Delta] C max the maximum value of the saturation degree differences, when the minimum value of the saturation difference and the [Delta] C min, and a maximum value of the saturation difference, the difference between the minimum value of the saturation difference | ΔC max -ΔC min | Is 2.8 ≦ | ΔC max −ΔC min | ≦ 19.6
Meet .
Condition 4:
The hue angle in the CIE 1976 L * a * b * color space of the above 15 kinds of modified Munsell color charts when the illumination by the spectral distribution of the target light is mathematically assumed is θ n (degrees) (where n
Is a natural number from 1 to 15)
CIE 1976 L * of the 15 types of modified Munsell color charts when mathematically assuming illumination with reference light selected according to the correlated color temperature T (K) of light emitted in the radiation direction
When the hue angle in the a * b * color space is θ nref (degree) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh n | is 0 ≦ | Δh n | ≦ 9. 0 (degrees) (n is a natural number from 1 to 15)
Meet.
However, it is set as ( DELTA) hn = (theta) n- ( theta ) nref .
条件3´´´:Condition 3 ″ ″:
下記式(3)で表される飽和度差の平均SAT Average SAT of saturation difference represented by the following formula (3) avav が下記式(4)を満たす。Satisfies the following formula (4).
波長をλ(nm)とし、 Let the wavelength be λ (nm),
当該発光要素から主たる放射方向に出射される光の分光分布をΦ The spectral distribution of the light emitted from the light emitting element in the main radiation direction is Φ elmelm (λ)、当該発光装置から主たる放射方向に出射される光の分光分布をφ(Λ), the spectral distribution of light emitted from the light emitting device in the main radiation direction is φ SSLSSL (λ)とし、(Λ)
Φ Φ elmelm (λ)は下記条件1と条件2の少なくともいずれか一方を満たさず、φ(Λ) does not satisfy at least one of the following conditions 1 and 2, and φ SSLSSL
(λ)は下記条件1と条件2をともに満たすことを特徴とする発光装置。(Λ) satisfies both the following conditions 1 and 2 as a light emitting device.
条件1:Condition 1:
対象となる光の分光分布におけるANSI C78.377で定義される黒体放射軌跡からの距離D Distance D from the blackbody radiation locus defined in ANSI C78.377 in the spectral distribution of the light of interest uvuv が、−0.0350 ≦ DIs -0.0350 ≦ D uvuv < 0となる光を含む。 <Includes light that becomes zero.
条件2:Condition 2:
対象となる光の分光分布をφ(λ)、対象となる光の分光分布の相関色温度T(K)に応じて選択される基準の光の分光分布をφ The spectral distribution of the target light is φ (λ), and the spectral distribution of the reference light selected according to the correlated color temperature T (K) of the spectral distribution of the target light is φ refref (λ)、対象となる光の分光分布の三刺激値を(X、Y、Z)、前記T(K)に応じて選択される基準の光の三刺激値を(X(Λ), the tristimulus value of the spectral distribution of the target light is (X, Y, Z), the tristimulus value of the reference light selected according to the T (K) is (X refref 、Y, Y refref 、Z, Z refref )とし、)age,
対象となる光の規格化分光分布S(λ)と、基準の光の規格化分光分布S The normalized spectral distribution S (λ) of the target light and the normalized spectral distribution S of the reference light refref (λ)と、これら規格化分光分布の差ΔS(λ)をそれぞれ、(Λ) and the difference ΔS (λ) between these normalized spectral distributions,
S(λ)=φ(λ)/Y S (λ) = φ (λ) / Y
S S refref (λ)=φ(Λ) = φ refref (λ)/Y(Λ) / Y refref
ΔS(λ)=S ΔS (λ) = S refref (λ)−S(λ)(Λ) −S (λ)
と定義し、And define
波長380nm以上780nm以内の範囲で、S(λ)の最長波長極大値を与える波長をλ The wavelength that gives the longest wavelength maximum of S (λ) within the wavelength range of 380 nm to 780 nm is λ. RR (nm)とした際に、(Nm)
λ λ RR よりも長波長側にS(λLonger than S (λ RR )/2となる波長Λ4が存在する場合においては下記数式(1)で表される指標A) / 2, where there is a wavelength Λ4, the index A expressed by the following formula (1) cgcg が−360 ≦ A-360 ≦ A cg cg ≦ −10を満たし、一方、≦ −10, while
λ λ RR よりも長波長側にS(λLonger than S (λ RR )/2となる波長Λ4が存在しない場合においては下記数式(2)で表される指標A) / 2, when there is no wavelength Λ4, the index A expressed by the following formula (2) cgcg が、−360 ≦ AIs -360 ≦ A cg cg ≦ −10を満たす。≦ −10 is satisfied.
条件3´:Condition 3 ′:
対象となる光の分光分布による照明を数学的に仮定した場合の#01から#15の下記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the following 15 types of modified Munsell color charts from # 01 to # 15 when the illumination by the spectral distribution of the target light is mathematically assumed ** aa ** bb ** 色空間におけるaA in color space ** 値、bValue, b **
値をそれぞれaEach value is a ** nn 、b, B ** nn (ただしnは1から15の自然数)とし、(Where n is a natural number from 1 to 15)
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 types of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T (K) of the light emitted in the radiation direction is mathematically assumed. **
aa ** bb ** 色空間におけるaA in color space ** 値、bValue, b ** 値をそれぞれaEach value is a ** nrefnref 、b, B ** nrefnref (ただしnは1から15の自然数)とした場合に、飽和度差ΔC(Where n is a natural number from 1 to 15), the saturation difference ΔC nn がBut
−3.8 ≦ ΔC −3.8 ≦ ΔC n n ≦ 18.6 (nは1から15の自然数)≦ 18.6 (n is a natural number from 1 to 15)
を満たす。Meet.
ただし、ΔC However, ΔC nn =√{(a= √ {(a ** nn )) 22 +(b+ (B ** nn )) 22 }−√{(a} -√ {(a ** nrefnref )) 22 +(b+ (B ** nrnr
efef )) 22 }とする。}.
15種類の修正マンセル色票 15 kinds of modified Munsell color chart
#01 7.5 P 4 /10 # 01 7.5 P 4/10
#02 10 PB 4 /10 # 02 10 PB 4/10
#03 5 PB 4 /12 # 03 5 PB 4/12
#04 7.5 B 5 /10 # 04 7.5 B 5/10
#05 10 BG 6 / 8 # 05 10 BG 6/8
#06 2.5 BG 6 /10 # 06 2.5 BG 6/10
#07 2.5 G 6 /12 # 07 2.5 G 6/12
#08 7.5 GY 7 /10 # 08 7.5 GY 7/10
#09 2.5 GY 8 /10 # 09 2.5 GY 8/10
#10 5 Y 8.5/12 # 10 5 Y 8.5 / 12
#11 10 YR 7 /12 # 11 10 YR 7/12
#12 5 YR 7 /12 # 12 5 YR 7/12
#13 10 R 6 /12 # 13 10 R 6/12
#14 5 R 4 /14 # 14 5 R 4/14
#15 7.5 RP 4 /12 # 15 7.5 RP 4/12
条件3´´:Condition 3 ″:
飽和度差の最大値をΔC The maximum value of the saturation difference is ΔC maxmax 、飽和度差の最小値をΔC, The minimum value of saturation difference is ΔC minmin とした場合に、飽和度差の最大値と、飽和度差の最小値との間の差|ΔCThe difference between the maximum value of the saturation difference and the minimum value of the saturation difference | ΔC maxmax −ΔC-ΔC minmin |が|
2.8 ≦ |ΔC 2.8 ≤ | ΔC maxmax −ΔC-ΔC minmin | ≦ 19.6| ≦ 19.6
を満たす。Meet.
条件4:Condition 4:
対象となる光の分光分布による照明を数学的に仮定した場合の上記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the above-mentioned 15 kinds of modified Munsell color charts when the illumination by the spectral distribution of the target light is mathematically assumed ** aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nn (度)(ただしn(Degree) (however, n
は1から15の自然数)とし、Is a natural number from 1 to 15)
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 types of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T (K) of the light emitted in the radiation direction is mathematically assumed. **
aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nrefnref (度)(ただしnは1から15の自然数)とした場合に、色相角差の絶対値|Δh(Degree) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh nn |が|
0 ≦ |Δh 0 ≦ | Δh nn | ≦ 9.0(度)(nは1から15の自然数)| ≦ 9.0 (degrees) (n is a natural number from 1 to 15)
を満たす。Meet.
ただし、Δh However, Δh nn =θ= Θ nn −θ−θ nrefnref とする。And
条件3´´´:Condition 3 ″ ″:
下記式(3)で表される飽和度差の平均SAT Average SAT of saturation difference represented by the following formula (3) avav が下記式(4)を満たす。Satisfies the following formula (4).
波長をλ(nm)とし、 Let the wavelength be λ (nm),
当該発光要素から主たる放射方向に出射される光の分光分布をΦ The spectral distribution of the light emitted from the light emitting element in the main radiation direction is Φ elmelm (λ)、当該発光装置から主たる放射方向に出射される光の分光分布をφ(Λ), the spectral distribution of light emitted from the light emitting device in the main radiation direction is φ SSLSSL (λ)とし、(Λ)
Φ Φ elmelm (λ)は下記条件1と条件3´をともに満たし、φ(Λ) satisfies both condition 1 and condition 3 ′ below, and φ SSLSSL (λ)も下記条件1と条件3´をともに満たすことを特徴とする発光装置。(Λ) also satisfies the following condition 1 and condition 3 ′.
条件1:Condition 1:
対象となる光の分光分布におけるANSI C78.377で定義される黒体放射軌跡からの距離D Distance D from the blackbody radiation locus defined in ANSI C78.377 in the spectral distribution of the light of interest uvuv が、−0.0350 ≦ DIs -0.0350 ≦ D uvuv < 0となる光を含む。 <Includes light that becomes zero.
条件3´:Condition 3 ′:
対象となる光の分光分布による照明を数学的に仮定した場合の#01から#15の下記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the following 15 types of modified Munsell color charts from # 01 to # 15 when the illumination by the spectral distribution of the target light is mathematically assumed ** aa ** bb ** 色空間におけるaA in color space ** 値、bValue, b **
値をそれぞれaEach value is a ** nn 、b, B ** nn (ただしnは1から15の自然数)とし、(Where n is a natural number from 1 to 15)
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 types of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T (K) of the light emitted in the radiation direction is mathematically assumed. **
aa ** bb ** 色空間におけるaA in color space ** 値、bValue, b ** 値をそれぞれaEach value is a ** nrefnref 、b, B ** nrefnref (ただしnは1から15の自然数)とした場合に、飽和度差ΔC(Where n is a natural number from 1 to 15), the saturation difference ΔC nn がBut
−3.8 ≦ ΔC −3.8 ≦ ΔC n n ≦ 18.6 (nは1から15の自然数)≦ 18.6 (n is a natural number from 1 to 15)
を満たす。Meet.
ただし、ΔC However, ΔC nn =√{(a= √ {(a ** nn )) 22 +(b+ (B ** nn )) 22 }−√{(a} -√ {(a ** nrefnref )) 22 +(b+ (B ** nrnr
efef )) 22 }とする。}.
15種類の修正マンセル色票 15 kinds of modified Munsell color chart
#01 7.5 P 4 /10 # 01 7.5 P 4/10
#02 10 PB 4 /10 # 02 10 PB 4/10
#03 5 PB 4 /12 # 03 5 PB 4/12
#04 7.5 B 5 /10 # 04 7.5 B 5/10
#05 10 BG 6 / 8 # 05 10 BG 6/8
#06 2.5 BG 6 /10 # 06 2.5 BG 6/10
#07 2.5 G 6 /12 # 07 2.5 G 6/12
#08 7.5 GY 7 /10 # 08 7.5 GY 7/10
#09 2.5 GY 8 /10 # 09 2.5 GY 8/10
#10 5 Y 8.5/12 # 10 5 Y 8.5 / 12
#11 10 YR 7 /12 # 11 10 YR 7/12
#12 5 YR 7 /12 # 12 5 YR 7/12
#13 10 R 6 /12 # 13 10 R 6/12
#14 5 R 4 /14 # 14 5 R 4/14
#15 7.5 RP 4 /12 # 15 7.5 RP 4/12
条件3´´:Condition 3 ″:
飽和度差の最大値をΔC The maximum value of the saturation difference is ΔC maxmax 、飽和度差の最小値をΔC, The minimum value of saturation difference is ΔC minmin とした場合に、飽和度差の最大値と、飽和度差の最小値との間の差|ΔCThe difference between the maximum value of the saturation difference and the minimum value of the saturation difference | ΔC maxmax −ΔC-ΔC minmin |が|
2.8 ≦ |ΔC 2.8 ≤ | ΔC maxmax −ΔC-ΔC minmin | ≦ 19.6| ≦ 19.6
を満たす。Meet.
条件4:Condition 4:
対象となる光の分光分布による照明を数学的に仮定した場合の上記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the above-mentioned 15 kinds of modified Munsell color charts when the illumination by the spectral distribution of the target light is mathematically assumed ** aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nn (度)(ただしn(Degree) (however, n
は1から15の自然数)とし、Is a natural number from 1 to 15)
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 types of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T (K) of the light emitted in the radiation direction is mathematically assumed. **
aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nrefnref (度)(ただしnは1から15の自然数)とした場合に、色相角差の絶対値|Δh(Degree) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh nn |が|
0 ≦ |Δh 0 ≦ | Δh nn | ≦ 9.0(度)(nは1から15の自然数)| ≦ 9.0 (degrees) (n is a natural number from 1 to 15)
を満たす。Meet.
ただし、Δh However, Δh nn =θ= Θ nn −θ−θ nrefnref とする。And
条件3´´´:Condition 3 ″ ″:
下記式(3)で表される飽和度差の平均SAT Average SAT of saturation difference represented by the following formula (3) avav が下記式(4)を満たす。Satisfies the following formula (4).
波長をλ(nm)とし、
当該発光要素から主たる放射方向に出射される光の分光分布をΦelm(λ)、当該発光装置から主たる放射方向に出射される光の分光分布をφSSL(λ)とし、
Φelm(λ)は下記条件1と条件2をともに満たし、φSSL(λ)も下記条件1と条件2をともに満たすことを特徴とする発光装置。
条件1:
対象となる光の分光分布におけるANSI C78.377で定義される黒体放射軌跡からの距離Duvが、−0.0350 ≦ Duv < 0となる光を含む。
条件2:
対象となる光の分光分布をφ(λ)、対象となる光の分光分布の相関色温度T(K)に応じて選択される基準の光の分光分布をφref(λ)、対象となる光の分光分布の三刺激値を(X、Y、Z)、前記T(K)に応じて選択される基準の光の三刺激値を(Xref、Yref、Zref)とし、
対象となる光の規格化分光分布S(λ)と、基準の光の規格化分光分布Sref(λ)と、これら規格化分光分布の差ΔS(λ)をそれぞれ、
S(λ)=φ(λ)/Y
Sref(λ)=φref(λ)/Yref
ΔS(λ)=Sref(λ)−S(λ)
と定義し、
波長380nm以上780nm以内の範囲で、S(λ)の最長波長極大値を与える波長をλR(nm)とした際に、
λRよりも長波長側にS(λR)/2となる波長Λ4が存在する場合においては下記数式(1)で表される指標Acgが−360 ≦ Acg ≦ −10を満たし、一方、
λRよりも長波長側にS(λR)/2となる波長Λ4が存在しない場合においては下記数式(2)で表される指標Acgが、−360 ≦ Acg ≦ −10を満たす。
Let the wavelength be λ (nm),
The spectral distribution of the light emitted from the light emitting element in the main radiation direction is Φ elm (λ), the spectral distribution of the light emitted from the light emitting device in the main radiation direction is φ SSL (λ),
Φ elm (λ) satisfies both condition 1 and condition 2 below, and φ SSL (λ) also satisfies both condition 1 and condition 2 below.
Condition 1:
Including the light in which the distance D uv from the black body radiation locus defined in ANSI C78.377 in the spectral distribution of the target light is −0.0350 ≦ D uv <0 .
Condition 2:
The target light spectral distribution is φ (λ), the reference light spectral distribution selected according to the correlated color temperature T (K) of the target light spectral distribution is φ ref (λ), and the target light is distributed. The tristimulus values of the spectral distribution of light are (X, Y, Z), the reference tristimulus values of the light selected according to T (K) are (X ref , Y ref , Z ref ),
The normalized spectral distribution S (λ) of the target light, the normalized spectral distribution S ref (λ) of the reference light, and the difference ΔS (λ) between these normalized spectral distributions, respectively,
S (λ) = φ (λ) / Y
S ref (λ) = φ ref (λ) / Y ref
ΔS (λ) = S ref (λ) −S (λ)
And define
When the wavelength giving the longest wavelength maximum value of S (λ) is λ R (nm) in the wavelength range of 380 nm to 780 nm,
When there is a wavelength Λ4 that is S (λ R ) / 2 on the longer wavelength side than λ R, the index A cg represented by the following formula (1) satisfies −360 ≦ A cg ≦ −10, ,
When there is no wavelength Λ4 that becomes S (λ R ) / 2 on the longer wavelength side than λ R, the index A cg represented by the following formula (2) satisfies −360 ≦ A cg ≦ −10.
条件3´:
対象となる光の分光分布による照明を数学的に仮定した場合の#01から#15の下記15種類の修正マンセル色票のCIE 1976 L*a*b*色空間におけるa*値、b*
値をそれぞれa* n、b* n(ただしnは1から15の自然数)とし、
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L*
a*b*色空間におけるa*値、b*値をそれぞれa* nref、b* nref(ただしnは1から15の自然数)とした場合に、飽和度差ΔCnが
−3.8 ≦ ΔCn ≦ 18.6 (nは1から15の自然数)
を満たす。
ただし、ΔCn=√{(a* n)2+(b* n)2}−√{(a* nref)2+(b* nr
ef)2}とする。
15種類の修正マンセル色票
#01 7.5 P 4 /10
#02 10 PB 4 /10
#03 5 PB 4 /12
#04 7.5 B 5 /10
#05 10 BG 6 / 8
#06 2.5 BG 6 /10
#07 2.5 G 6 /12
#08 7.5 GY 7 /10
#09 2.5 GY 8 /10
#10 5 Y 8.5/12
#11 10 YR 7 /12
#12 5 YR 7 /12
#13 10 R 6 /12
#14 5 R 4 /14
#15 7.5 RP 4 /12 A light emitting device according to claim 11, Φ elm (λ) is 'meets, φ SSL (λ) be the following condition 3' following condition 3 light emitting device, wherein the full-plus that the.
Condition 3 ′ :
CIE 1976 L * a * b * a * value in color space, b * of the following 15 types of modified Munsell color charts from # 01 to # 15 when the illumination by the spectral distribution of the target light is mathematically assumed
The values are a * n and b * n (where n is a natural number from 1 to 15),
CIE 1976 L * of the 15 types of modified Munsell color charts when mathematically assuming illumination with reference light selected according to the correlated color temperature T (K) of light emitted in the radiation direction
a * b * a * values in a color space, b * values of each a * nref, b * nref (where n is from 1 natural numbers 15) when the degree of saturation difference [Delta] C n is -3.8 ≦ [Delta] C n ≦ 18.6 (n is a natural number from 1 to 15)
The full-plus.
However, ΔC n = √ {(a * n ) 2 + (b * n ) 2 } −√ {(a * nref ) 2 + (b * nr
ef ) 2 }.
15 types of modified Munsell color chart # 01 7.5 P 4/10
# 02 10 PB 4/10
# 03 5 PB 4/12
# 04 7.5 B 5/10
# 05 10 BG 6/8
# 06 2.5 BG 6/10
# 07 2.5 G 6/12
# 08 7.5 GY 7/10
# 09 2.5 GY 8/10
# 10 5 Y 8.5 / 12
# 11 10 YR 7/12
# 12 5 YR 7/12
# 13 10 R 6/12
# 14 5 R 4/14
# 15 7.5 RP 4/1 2
条件3´´:Condition 3 ″:
飽和度差の最大値をΔC The maximum value of the saturation difference is ΔC maxmax 、飽和度差の最小値をΔC, The minimum value of saturation difference is ΔC minmin とした場合に、飽和度差の最大値と、飽和度差の最小値との間の差|ΔCThe difference between the maximum value of the saturation difference and the minimum value of the saturation difference | ΔC maxmax −ΔC-ΔC minmin |が|
2.8 ≦ |ΔC 2.8 ≤ | ΔC maxmax −ΔC-ΔC minmin | ≦ 19.6| ≦ 19.6
を満たす。Meet.
条件4:Condition 4:
対象となる光の分光分布による照明を数学的に仮定した場合の上記15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the above-mentioned 15 kinds of modified Munsell color charts when the illumination by the spectral distribution of the target light is mathematically assumed ** aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nn (度)(ただしn(Degree) (however, n
は1から15の自然数)とし、Is a natural number from 1 to 15)
当該放射方向に出射される光の相関色温度T(K)に応じて選択される基準の光での照明を数学的に仮定した場合の当該15種類の修正マンセル色票のCIE 1976 L CIE 1976 L of the 15 types of modified Munsell color charts when the illumination with the reference light selected according to the correlated color temperature T (K) of the light emitted in the radiation direction is mathematically assumed. **
aa ** bb ** 色空間における色相角をθThe hue angle in the color space is θ nrefnref (度)(ただしnは1から15の自然数)とした場合に、色相角差の絶対値|Δh(Degree) (where n is a natural number from 1 to 15), the absolute value of the hue angle difference | Δh nn |が|
0 ≦ |Δh 0 ≦ | Δh nn | ≦ 9.0(度)(nは1から15の自然数)| ≦ 9.0 (degrees) (n is a natural number from 1 to 15)
を満たす。Meet.
ただし、Δh However, Δh nn =θ= Θ nn −θ−θ nrefnref とする。And
条件3´´´:Condition 3 ″ ″:
下記式(3)で表される飽和度差の平均SAT Average SAT of saturation difference represented by the following formula (3) avav が下記式(4)を満たす。Satisfies the following formula (4).
当該発光要素から主たる放射方向に出射される光の分光分布から導出されるDuvをDuv(Φelm)、当該発光装置から主たる放射方向に出射される光の分光分布から導出されるDuvをDuv(φSSL)と定義した場合に、
Duv(φSSL)<Duv(Φelm)
を満たすことを特徴とする発光装置。 The light-emitting device according to claim 1 , 4, 8 or 11 ,
D uv derived from the light-emitting derived from the spectral distribution of the light emitted in the main radiation direction from the element D uv a D uv (Φ elm), the spectral distribution of the light emitted from the light-emitting device in the main radiation direction Is defined as D uv (φ SSL ),
D uv (φ SSL ) <D uv (Φ elm )
A light emitting device characterized by satisfying the above.
当該発光要素から主たる放射方向に出射される光の分光分布から導出されるAcgをAcg(Φelm)、当該発光装置から主たる放射方向に出射される光の分光分布から導出されるAcgをAcg(φSSL)と定義した場合に、
Acg(φSSL)<Acg(Φelm)
を満たすことを特徴とする発光装置。 The light-emitting device according to claim 4 or 11 ,
The A cg derived from the spectral distribution of the light emitted from the light-emitting element in the principal radiating direction A cg (Φ elm), A cg derived from the spectral distribution of the light emitted from the light-emitting device in the main radiation direction Is defined as A cg (φ SSL ),
A cg (φ SSL ) <A cg (Φ elm )
A light emitting device characterized by satisfying the above.
当該発光要素から主たる放射方向に出射される光の分光分布から導出される前記飽和度差の平均をSATav(Φelm)、
当該発光装置から主たる放射方向に出射される光の分光分布から導出される前記飽和度
差の平均をSATav(φSSL)と定義した場合に、
SATav(Φelm)<SATav(φSSL)
を満たすことを特徴とする発光装置。 The light emitting device according to claim 3, 7, 10 or 14 ,
SAT av (Φ elm ), the average of the saturation differences derived from the spectral distribution of the light emitted from the light emitting element in the main radiation direction,
When the average of the saturation differences derived from the spectral distribution of light emitted in the main radiation direction from the light emitting device is defined as SAT av (φ SSL ),
SAT av (Φ elm ) <SAT av (φ SSL )
A light emitting device characterized by satisfying the above.
前記発光装置から当該放射方向に出射される光は、分光分布φSSL(λ)から導出される波長380nm以上780nm以下の範囲の放射効率K(lm/W)が
180(lm/W) ≦ K(lm/W) ≦ 320(lm/W)
を満たすことを特徴とする発光装置。 The light-emitting device according to any one of claims 1 to 20 ,
The light emitted from the light emitting device in the radiation direction has a radiation efficiency K (lm / W) in the range of 380 nm to 780 nm derived from the spectral distribution φ SSL (λ), 180 (lm / W) ≦ K (Lm / W) ≦ 320 (lm / W)
A light emitting device characterized by satisfying the above.
2550(K) ≦ T(K) ≦ 5650(K)
を満たすことを特徴とする発光装置。 A light emitting device according to any one of claims 1 to 21 correlated color temperature T as a light emitting device (K) is 2550 (K) ≦ T (K) ≦ 5650 (K)
A light emitting device characterized by satisfying the above.
nm以上75nm以下であることを特徴とする発光装置。 A light emitting device according to any one of claims 1 to 24, wherein the peak wavelength of the emission spectrum of the semiconductor light emitting element is less than the above 495 nm 590 nm, and the full width at half maximum 2
A light emitting device having a thickness of greater than or equal to nm and less than or equal to 75 nm.
よび(Ba,Sr,Ca,Mg)Si2O2N2:Euからなる群から選択される1種以上
を含むことを特徴とする発光装置。
(Ba,Sr,Ca)MgAl10O17:Mn,Eu (5)
SraBabEux(PO4)cXd (5)´
(一般式(5)´において、XはClである。また、c、d及びxは、2.7≦c≦3.3、0.9≦d≦1.1、0.3≦x≦1.2を満足する数である。さらに、a及びbは、a+b=5−xかつ0≦b/(a+b)≦0.6の条件を満足する。) 34. The light emitting device according to claim 33, wherein the phosphor is a phosphor represented by the following general formula (5), a phosphor represented by the following general formula (5) ′, (Sr, Ba) 3 MgSi. A light emitting device comprising at least one selected from the group consisting of 2 O 8 : Eu 2+ and (Ba, Sr, Ca, Mg) Si 2 O 2 N 2 : Eu.
(Ba, Sr, Ca) MgAl 10 O 17 : Mn, Eu (5)
Sr a Ba b Eu x (PO 4) c X d (5) '
(In the general formula (5) ′, X is Cl. Also, c, d and x are 2.7 ≦ c ≦ 3.3, 0.9 ≦ d ≦ 1.1, 0.3 ≦ x ≦. (In addition, a and b satisfy the condition of a + b = 5-x and 0 ≦ b / (a + b) ≦ 0.6.)
を特徴とする発光装置。
BaaCabSrcMgdEuxSiO4 (6)
(一般式(6)においてa、b、c、dおよびxが、a+b+c+d+x=2、1.0 ≦ a ≦ 2.0、0 ≦ b < 0.2、0.2 ≦ c ≦ 1.0、0 ≦ d < 0.2
および0 < x ≦ 0.5を満たす。)
Ba1-x-ySrxEuyMg1-zMnzAl10O17 (6)´
(一般式(6)´においてx、yおよびzはそれぞれ0.1≦x≦0.4、0.25≦y≦0.6及び0.05≦z≦0.5を満たす。) 36. The light emitting device according to claim 35, wherein the phosphor is represented by the following general formula (6): Si 6-z Al z O z N 8-z : Eu (where 0 <z <4.2). A phosphor represented by the following general formula (6) ′, and at least one selected from the group consisting of SrGaS 4 : Eu 2+ .
Ba a Ca b Sr c Mg d Eu x SiO 4 (6)
(In the general formula (6), a, b, c, d and x are a + b + c + d + x = 2, 1.0 ≦ a ≦ 2.0, 0 ≦ b <0.2, 0.2 ≦ c ≦ 1.0, 0 ≦ d <0.2
And 0 <x ≦ 0.5. )
Ba 1-xy Sr x Eu y Mg 1-z Mn z Al 10 O 17 (6) ′
(In the general formula (6) ′, x, y, and z satisfy 0.1 ≦ x ≦ 0.4, 0.25 ≦ y ≦ 0.6, and 0.05 ≦ z ≦ 0.5, respectively.)
はNaおよび/またはK;MはSiおよびAl;−1≦x≦1かつ0.9≦y+z≦1.1かつ0.001≦z≦0.4かつ5≦n≦7)、(Ca,Sr,Ba,Mg)AlSiN3:Euおよび/または(Ca,Sr,Ba)AlSiN3:Eu、並びに(CaAlSiN3)1-x(Si2N2O)x:Eu(ただし、xは0<x<0.5)からなる群から選択
される1種以上を含むことを特徴とする発光装置。
(La1-x-yEuxLny)2O2S (7)
(一般式(7)において、x及びyはそれぞれ0.02≦x≦0.50及び0≦y≦0.50を満たす数を表し、LnはY、Gd、Lu、Sc、Sm及びErの少なくとも1種の3価希土類元素を表す。)
(k−x)MgO・xAF2・GeO2:yMn4+ (7)´
(一般式(7)´において、k、x、yは、各々、2.8≦k≦5、0.1≦x≦0.7、0.005≦y≦0.015を満たす数を表し、Aはカルシウム(Ca)、ストロンチウム(Sr)、バリウム(Ba)、亜鉛(Zn)、またはこれらの混合物である。) 38. The light-emitting device according to claim 37, wherein the phosphor is represented by the following general formula (7), a phosphor represented by the following general formula (7) ′, (Sr, Ca, Ba) 2 Al x Si 5-x O x N 8-x: Eu ( provided that 0 ≦ x ≦ 2), Eu y (Sr, Ca, Ba) 1-y: Al 1 + x Si 4-x O x N 7- x (provided that 0 ≦ x <4,0 ≦ y < 0.2), K 2 SiF 6: Mn 4+, A 2 + x M y Mn z F n (A
Is Na and / or K; M is Si and Al; −1 ≦ x ≦ 1 and 0.9 ≦ y + z ≦ 1.1 and 0.001 ≦ z ≦ 0.4 and 5 ≦ n ≦ 7), (Ca, Sr, Ba, Mg) AlSiN 3 : Eu and / or (Ca, Sr, Ba) AlSiN 3 : Eu and (CaAlSiN 3 ) 1-x (Si 2 N 2 O) x : Eu (where x is 0 < A light-emitting device comprising at least one selected from the group consisting of x <0.5).
(La 1-xy Eu x Ln y) 2 O 2 S (7)
(In the general formula (7), x and y represent numbers satisfying 0.02 ≦ x ≦ 0.50 and 0 ≦ y ≦ 0.50, respectively, and Ln represents Y, Gd, Lu, Sc, Sm and Er. Represents at least one trivalent rare earth element)
(K−x) MgO.xAF 2 .GeO 2 : yMn 4+ (7) ′
(In general formula (7) ′, k, x, and y represent numbers satisfying 2.8 ≦ k ≦ 5, 0.1 ≦ x ≦ 0.7, and 0.005 ≦ y ≦ 0.015, respectively. , A is calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), or a mixture thereof.
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EP2739704B1 (en) * | 2011-08-04 | 2015-10-14 | Koninklijke Philips N.V. | Light converter and lighting unit comprising such light converter |
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2014
- 2014-03-04 JP JP2014041321A patent/JP6271301B2/en active Active
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2017
- 2017-12-27 JP JP2017251523A patent/JP6462841B2/en active Active
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2018
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