Материал: Weber H., Herziger G., Poprawe R. (eds.) Laser Fundamentals. Part 1 (Springer 2005)(263s) PEo

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B¨ornstein-Landolt

VIII/1A1 Series New

Table 4.1.31 continued.

Crystal	θpm, type of	λpump	Ithr	λOPO	τp	η	Ref.	Notes
	interaction	[µm]	[MW cm−2]	[µm]	[ps]	[%]
LBO	θ = 90 ◦ , ϕ = 0 ◦	0.5235	1100	0.909–1.235	33	50	[93Hal1,	DROPO, T = 167–180 ◦ C
			(4.5 mW)				92Ebr1]
	θ = 90 ◦ , ϕ = 0 ◦	0.5235	15 (30 mW)	0.65–2.65	1.7	50	[93Hal1]	DROPO, L = 12 mm, P = 0.21 W
	ooe, θ = 90 ◦ ,	0.5235	47 mW	0.839–1.392	1.8	70 a	[94Rob1] SP SROPO, P = 88 mW, L = 3 mm
	ϕ = 0 ◦					75 a
	ooe, θ = 90 ◦ ,	0.5235	170 mW	0.65–2.7	1.63	75 a	[95But]	SP OPO, P = 210 mW, L = 15 mm
	ϕ = 0 ◦
	θ = 90 ◦ , ϕ = 0 ◦	0.523	100	0.72–1.91	1	34	[93McC1] SP SROPO, L = 13 mm, T = 125–175 ◦ C,
	θ = 90 ◦ , ϕ = 0 ◦					27 (75 a) [93But]		Pav = 89 mW
	θ = 90 ◦ , ϕ = 0 ◦	0.523	80 (70 mW)	0.8–1.5	1.2–1.5	27 (75 a) [93But]		SROPO, L = 12 mm, Pav = 78 mW
	θ = 90 ◦ ,	0.355	–	0.46–1.6	15	30	[91Zha]	Injection seeding from OPO, L = 16 mm,
	ϕ = 27–43 ◦							I0 = 2.8 GW cm−2, E = 0.3 mJ
	θ = 90 ◦ ,	0.355	–	0.403–2.58	12	28	[92Kra]	TWOPO, L1 = L2 = 15 mm, I0 = 5 GW cm−2,
	ϕ = 18–42 ◦							E = 0.1–1 mJ
	θ = 0 ◦ , ϕ = 0 ◦	0.355	2300	0.4159–	30	38	[92Hua,	TWOPO, L = 10 mm, T = 21–450 ◦ C,
	θ = 90 ◦ ,			0.4826			93Hua]	I0 = 18 GW cm−2, ∆ λ = 0.15 nm
	θ = 90 ◦ ,	0.355	1000	0.452–1.65	9	26	[93Agn]	DROPO, L = 10.5 mm, E = 0.15 mJ
	ϕ = 30–42 ◦
KTP	θ = 82–90 ◦ ,	1.064	0.8 W	1.57–1.59;	2–3	15	[93Chu]	SROPO, L = 10 mm, f = 75 MHz,
	ϕ = 0 ◦			3.21–3.30				∆ λ = 1.5 nm
	–	1.064		2.128	100	25	[93Lot]	SP OPO with 6 KTP (total length 58 mm),
								P = 14 W
	θ = 81–90 ◦ ,	1.053	5.8 W	1.55–1.56;	12	21	[93Gra]	SP OPO, L = 6 mm, P = 2 W
	ϕ = 0 ◦			3.22–3.28
	θ = 40.6–45.2 ◦ ,	0.8	–	1.02–1.16;	2.6	–	[95Gra]	OPA, E = 0.04 mJ
	ϕ = 0 ◦ , oeo			2.6–3.7
	θ = 53 ◦ , ϕ = 0 ◦ ,	0.72–0.85	0.8 W	1.44–1.64	1.1	20	[96Qia]	SP SROPO, P = 200 mW, L = 7 mm

oeo

(continued)

182

oscillation parametric Optical 7.1.4

187 .p .[Ref

B¨ornstein-Landolt

VIII/1A1 Series New

Table 4.1.31 continued.

Crystal	θpm, type of	λpump	Ithr	λOPO	τp	η	Ref.	Notes
	interaction	[µm]	[MW cm−2]	[µm]	[ps]	[%]
KTP	θ = 90 ◦ , ϕ = 0 ◦	0.72–0.853	150	1.052–1.214;	1.2	42	[93Neb]	SP OPO, L = 6 mm, P = 0.7 W
				2.286–2.871
	θ = 54 ◦ , ϕ = 0 ◦ ,	0.532	250	0.614–4.16	0.39	12	[94Umb]	L = 14 mm
	eoo
	eoe, θ = 90 ◦ ,	0.527	0.9 W	0.851–0.938;	2.4–3.2	13	[95Che]	SROPO, P = 80–280 mW, L = 5 mm
	ϕ = 35 ◦			1.2–1.381
	θ = 40–70 ◦ ,	0.526	–	0.6–2.0	30	10	[88Van]	L = 20 mm
	ϕ = 90 ◦
	θ = 40–80 ◦ ,	0.526	–	0.6–4.3	30	10	[88Van]	L = 20 mm
	ϕ = 0 ◦					16 (79 a) [92McC]
	θ = 90 ◦ ,	0.523	57 (61 mW)	1.002–1.096	2.2	16 (79 a) [92McC]		SP OPO, L = 5 mm, P = 42 mW
	ϕ = 10–35 ◦					10 (56 a) [91Ebr1,
	–	0.5235	1000	0.946–1.02;	8	10 (56 a) [91Ebr1,		SP SROPO, L = 5 mm, P = 2 mW
			(2 mW)	1.075–1.172			93Hal1]
	θ = 90 ◦	0.523	60 (61 mW)	0.938–1.184	1–2	16	[93McC2] SROPO, L = 5 mm, f = 125 MHz, P = 40 mW
	θ = 90 ◦ ,	0.526	0.5 W	1.01–1.1	14	44	[93Gra]	SP OPO, L = 6 mm, P = 0.58 W
	ϕ = 0–33 ◦
KTA	θ = 90 ◦ , ϕ = 0 ◦	1.064	–	1.54; 3.47	7	75	[98Ruf]	SP OPO, L = 15 mm
Banana	θooe = 90 ◦	0.532	5	0.8–1.6	10	25	[83Oni]	SP OPO
	θooe = 90 ◦	0.53	50	0.65–3	10	5.3	[87Ion]	SP OPO, I0 = 250 MW cm−2
	θooe = 90 ◦	0.532	7–9	0.672–2.56	15–45	8.1	[89Pis,	SP SROPO, L = 10 mm, f = 139 MHz,
							90Pis]	T = 75–350 ◦ C
α–HIO3	eoe	0.532	–	0.7–2.2	30–45	10–12	[77Dan]	TWOPO, L1 = L2 = 2 cm, I0 = 4–5 GW cm−2
	eoe	0.527	60	–	5–6	10	[80Bar2]	SP OPO, ∆ ν ∆ τ = 0.7

a Pump depletion.

187] .p .Ref

crystals in conversion Frequency 1.4

183

B¨ornstein-Landolt

VIII/1A1 Series New

Table 4.1.32. Femtosecond OPO in the UV, visible, and near IR regions.

Crystal	θpm, type of	λpump	Ithr	λOPO	τp	η	Ref.	Notes
	interaction	[µm]	[MW cm−2]	[µm]	[fs]	[%]
BBO	θeoe = 28 ◦	0.78	–	1.1–2.6	60	35	[94Nis]	TWOPO, L1 = L2 = 4.8 mm, E = 0.15 mJ
	θooe = 20 ◦	0.8	–	1.2–1.3	70	5	[94Sei1]	TWOPO, L = 4 mm
	ooe	0.62	–	0.45–2.8	200	15	[91Joo]	TWOPO, L1 = 5 mm, L2 = 7 mm, E = 20 µJ
	ooe, eoe	0.6	–	0.75–3.1	180–250	23	[93Dan]	TWOPO-OPA, L1 = L2 = 8 mm,
								I0 = 70 GW cm−2
	θooe = 19.5–21 ◦	0.53	2200	0.68–2.4	75	30	[88Bro]	SP SROPO, L = 7.2 mm, I0 = 2.2 GW cm−2,
								E = 2 mJ
	ooe	0.527	–	0.7–1.8	65–260	3	[90Lae2,	SP SROPO, L = 5.8 mm
							91Lae,
							93Lae]	OPA with gain ratio 2 × 104
	ooe	0.527	–	1.04–1.07	70	–	[92Dub]	OPA with gain ratio 2 × 104
	θooe = 32 ◦	0.4	–	0.566–0.676	30	10	[94Dri]	SP OPO, P = 100 mW
	ooe	0.4	–	0.59–0.666	13	50	[95Gal2]	SP OPO, P = 130 mW
	ooe	0.395	–	0.55–0.69	14	–	[98Shi]	NC OPA, seeding with white light continuum
	θooe = 32 ◦	0.39	–	0.5–0.7	11	–	[97Cer]	OPA, seeding with white light continuum,
								L = 1 mm
LBO	–	0.8	–	1.1–2.4	40	38	[95Kaf]	SP OPO, L = 6 mm, P = 550 mW
	–	0.77–0.8	320	1.374–1.530;	720	7.5	[95Ebr2]	SP OPO, P = 90 mW
				1.676–1.828
	θ = 90 ◦ , ϕ = 0 ◦	0.605	–	0.85–0.97;	200	10–15	[93Dan,	TWOPO, L1 = L2 = L3 = 15 mm,
				1.6–2.1			93Ban]	T = 30–85 ◦ C, I0 = 25 GW cm−2
KTP	θ = 43 ◦ , ϕ = 0 ◦ ,	0.83	325 mW	1.05–1.16;	175	15 a	[95McC]	SP OPO, L = 2 mm
	eoo			2.9–4.0		55 a
	θ = 90 ◦ , ϕ = 0 ◦ ,	0.816	–	2.5–2.9	160	55 a	[95Hol]	SP OPO-OPA, L1 = L2 = 0.9 mm, E = 0.55 µJ
	eoo					55 a
	ϕ = 0 ◦	0.765–0.815	–	1.22–1.37;	57–135	55 a	[92Pel]	L = 1.15 mm, f = 90 MHz, P = 340 mW (135 fs)
				1.82–2.15				and 115 mW (57 fs)

(continued)

184

oscillation parametric Optical 7.1.4

187 .p .[Ref

B¨ornstein-Landolt

VIII/1A1 Series New

Table 4.1.32 continued.

Crystal	θpm, type of	λpump	Ithr	λOPO	τp	η	Ref.	Notes
	interaction	[µm]	[MW cm−2]	[µm]	[fs]	[%]
KTP	θ = 67 ◦ , ϕ = 0 ◦	0.765	40000;	1.2–1.34;	62	–	[92Fu]	SP OPO, L = 1.5 mm, f = 76 MHz, P = 175 mW
			(180 mW)	1.78–2.1
	–	0.745	100 mW	0.53–0.585	200	29	[97Kar]	SP OPO with ICSHG (self-doubling OPO)
	θ = 45 ◦ , ϕ = 0 ◦	0.68	–	1.16–2.2;	57	60 a	[93Pow1] L = 1.5 mm, P = 0.68 W, ICSHG in BBO
				0.58–0.657				(L = 47 µm)
	ϕ = 0 ◦	0.645	110 mW	1.2–1.34	220	13	[92Mak]	SP OPO, P = 30 mW
	θ = 53 ◦ , ϕ = 0 ◦	0.61	–	0.755–1.04;	105–120	–	[90Wac,	SP OPO in CPM dye laser cavity, L = 1.4 mm
				1.5–3.2			91Wac]
	θ = 62 ◦ , ϕ = 0 ◦ ,	0.524	2000	1.2–1.6	260	10	[95Rau]	SP OPO, L = 3 mm
	eoo
	θ = 62 ◦ , ϕ = 0 ◦	0.5235	–	1.2–1.7	300	–	[98Lae]	SP OPO, L = 6 mm, E = 10 nJ
KTA	ϕ = 0 ◦ , oeo	0.78	–	1.29–1.44;	85–150	10–15	[93Pow2] L = 1.47 mm, P = 75 mW
				1.83–1.91
RTA	θ = 53 ◦ , ϕ = 0 ◦ ,	0.76–0.82	–	1.03–1.3;	58	25	[94Pow]	SP SROPO, L = 1.8 mm, P = 250 mW
	eoo			2.15–3.65
	θ = 90 ◦ , ϕ = 0 ◦ ,	0.78–0.86	50 mW	1.33	70	32	[95Rei]	L = 2 mm, P = 185 mW
	eoo
	–	Ti:Sa	–	1.25; 2.25	78	33	[97Rei]	SP OPO, f = 344 MHz, P = 0.6 W
KNbO3	θ = 38 ◦ , ϕ = 90 ◦	0.78	–	2.3–5.2	60–90	23	[95Spe,	L = 1 mm, P = 170–300 mW
							96Spe]
NPP	–	0.62	–	0.8–1.6	150–290	–	[86Led,	L = 1.5 mm
							87Led]

a Pump depletion.

187] .p .Ref

crystals in conversion Frequency 1.4

185

186	4.1.8 Picosecond continuum generation	[Ref. p. 187

Table 4.1.33. Optical parametric oscillation in the mid IR region.

Crystal	λpump	λOPO	τp	Conversion	Ref.
	[µm]	[µm]		e ciency [%]

Ag3AsS3	1.065	1.82–2.56	26 ns	1	[72Han]
	1.064	1.2–8	8 ps	0.01–1	[83Els]
AgGaS2	1.064	1.2–10	8 ps	0.1–10	[84Els]
	1.06	1.4–4.0	18 ns	16	[84Fan]
	1.064	4.5–8.7	15–20 ps	5.4	[91Bak]
	1.064	1.16–12.9	19 ps	25	[93Kra]
	1.064	1.319; 5.505	45–80 ps	63 a	[94Che]
	1.047	2.6–7	0.5–2.6 ps	–	[98Lae]
	0.845	1.267; 2.535	cw	2	[98Dou]
	0.74–0.85	3.3–10	160 fs	20	[94Sei2]
AgGaSe2	2.05	2.65–9.02	30 ns	> 18	[86Eck]
	2.06	4.1	30 ns	23	[93Bud]
	1.57	6–14	6 ns	20	[97Cha]
	1.34	1.6–1.7; 6.7–6.9	30 ns	> 18	[86Eck]
ZnGeP2	2.94	5.51–5.38;	80 ps	5.3	[85Vod]
		6.29–6.46
	2.94	5–5.3; 5.9–6.3	150 ps	17	[87Vod]
	2.79	5.3; 5.9	100 ps	10	[93Vod2]
	2.8; 2.94	4–10	100 ps	1–18	[91Vod, 93Vod1, 95Vod2]
GaSe	2.8; 2.94	3.5–18	100 ps	1	[91Vod, 93Vod1, 95Vod1]
CdSe	1.833	9.8–10.4; 2.26–2.23	300 ns	40	[72Her]
	2.36	7.9–13.7	40 ns	15	[72Dav, 73Dav]
	2.87	4.3–4.5; 8.1–8.3	140 ns	15	[74Wei]
	2.87	14.1–16.4	–	–	[76Wen]

a Pump depletion.

4.1.8 Picosecond continuum generation

Table 4.1.34. Picosecond continuum generation in crystals.

Crystal	λpump	Ipump	λcont	η	Cut angle	Ref.
	[µm]	[109 W cm−2]	[µm]	[% ]	of crystals
KDP	1.054	50	0.3–1.1	10	θ = 49 ◦	[83Mur]
KDP	0.527	30–40	0.84–1.4	15	θ = 42 ◦	[82Bar]
LiIO3	0.355	–	0.46–1.55	–	θ = 90 ◦	[85Pok]
LiIO3	0.532	0.3	0.67–2.58	–	θ = 90 ◦	[85Pok]
LiIO3	1.064	–	1.72–3.0	–	θ = 90 ◦	[85Pok]
LiNbO3	1.064	–	1.92–2.38	3	θ = 44.7 ◦	[75Cam]
GaAs	9.3	100	3–14	–	–	[85Cor]

Landolt-B¨ornstein

New Series VIII/1A1

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