LUMINESCENT SILICATE, LUMINESCENT SCREENS AND LAMPS COMPRISING SUCH A LUMINESCENT SILICATE

Abstract: A luminescent silicate having a composition defined by the formula Me 3-p-q Pb p Mn q Ln 2-r-x-y-z Gd r Ce x Tb y Dy z Si₆ O₁₈, wherein Me represents Sr and/or Ca and Ln represents Y and/or La, wherein, if q = r = x = y = z = 0, it holds that 0.01 ≦ p ≦ 0.50 wherein, if p = q = y = z = 0, it holds that 0.01 ≦ x ≦ 0.80 and 0 ≦ r ≦ 2-x wherein, if q = x = y = z = 0, it holds that 0.01 ≦ p ≦ 0.50 and 0.05 ≦ r ≦ 2.0; and wherein otherwise is holds that 0.01 ≦ p ≦ 0.50 0.05 ≦ r ≦ 2-x-y-z 0 ≦ q ≦ 0.30 0 ≦ x ≦ 0.80 0 ≦ y ≦ 1.0 0 ≦ z ≦ 0.10 0.005 ≦ q + x + y + z.

Description: "Luminescent silicate, luminescent screens and lamps comprising such a luminescent silicate." The invention relates to a luminescent silicate of an alkaline earth metal together with yttrium and/or lanthanum. In addition, the invention relates to a luminescent screen comprising such a luminescent silicate and to a low-pressure mercury discharge lamp having such a luminescent screen. Luminescent silicates of an alkaline earth metal together with yttrium or lanthanum are known from Netherlands Patent Application 7005708 (PHN 4817). Said application describes such silicates, the crystal structure of which corresponds to the crystal structure of apatite. Efficiently luminescing materials are obtained on activation of these materials by antimony, lead and/or tin. The publication of Dokl.- Akad. Nauk SSSR 243 (1978), 891 discloses a number of silicates which are defined by the formula Me3IIMe2III Si6O18, wheren MeII represents Sr or Ca and Me represents Y or an element of the lanthanum series. It appears that these compounds are crystalline materials having a triclinic crystal structure. Object of the invention is to provide novel luminescent materials which have very advantageous properties when used in a luminescent screen. According to the invention a luminescent silicate of an alkaline earth metal together with yttrium and/or lanthanum is characterized in that the silicate has a composition defined by the formula Me3-p-q Pbp Mnq In2-r-x-y-z GdrCex Tby Dyz Si6 O18 wherein Me represents strontium and/or calcium and Ln represents yttrium and/or lanthanum, wherein, if q=r=x=y=z=O, it holds that 0.01#p#0.50 wherein, if p=q=y=z=O, it holds that 0.01# x#0.80 and O#r#2-x, wherein, if q=x=y=z=O it holds that 0.01#p#0.50 and 0.05#r#2.0 and wherein otherwise it holds that 0.01#p#0.50 0.05#r#2-x-y-z 0#q#0.30 0#x#0.80 0#y#1.0 0#z#0.10 0.005 $ q+xty+z It appeared that from the group of silicate compounds having a triclinic crystal structure the silicates of Sr and/or Ca together with Y and/or La are suitable host lattices for activation by at least one of the elements Pb, Mn, Gd, Ce, Tb and Dy. The luminescent materials then obtained can be properly excited, for examply by ultra-violet radiation, in particular by short-wave ultra-violet radiation, and then luminesce in a very efficient manner. The choice of the elements to be used for Me and for Ln do nt appear to be critical as these elements have very little influence on the luminescent properties. The above-mentioned activators can be used alone or combine, very different emissions being obtained, which are very advantageous for practical uses, depending on the choice of the activator(s). The concentrations of the activators, denoted by the indices p, q, r, x, y and z, are located within predetermined limits. In order to obtain a sufficient absorption of excitation energy and/or a sufficiently high quantum efficiency an activator is not used in a concentration below a predetermined minimum value. A predetermined maximum concentration of an activator is not exceeded to avoid the radiation efficiency from being reduced unacceptably by concentration quenching. If the silicates are activated by lead alone (q=r=x=y=z=O) materials are obtained having very short-wave length lead emission with a maximum at approx. 302 nm. The lead which replaces a portion of the Me is then chosen in a concentration, p, of,not less than 0.01 and not more than 0.50. On activation by cerium along (p=q=y=z=O) materials are obtained which emit in the near part of the ultraviolet spectrum with a maximum of the emission band at 385- & 0 nm. It appeared that these materials may contain gadolinium (04 ri 2-x) as this element does not act as an activator element for these materials, but may occur as a lattice component (in a Ln site). The cerium concentration, x, is chosen in the range from 0.01 to 0.80. Silicates according to the invention which cCjn- tain both lead and gadolinium are very efficient emitters of the characteristic Gd-radiation (line emission at approximately 313 nm). In these materials the excitation energy, for example the 254 nm-radiation of a low-pressure mercury vapour discharge lamp, is absorbed by the lead and is transferred to the gadolinium. The lead content, p, is again chosen in a range from 0.01 to 0.50. The gadolinium content, r, may be chosen between very wide limits (0.05#r#2) as then concentration quenching does not occur to a substantial extent. On activation of the silicates by a third ac activator element (Mn, Ce, Tb and/or Dy) in addition to Pb (0.014 pg 0.50) and Gd (0.05g rg 2-x-y-z) materials are obtained having the characteristic emission of the third activator element, the minimum value of the concentration of this third activator element being 0.005 (q, x, y or z). In these materials the Gd plays an intermediate part in the transfer of excitation energy of the Pb to the third activator element via Gd. If Mn is chosen as the third activator, the Mn content q being not more than 0.30, materials are obtained having a green emission band with a maximum at approximately 550 nm. The use of cerium (x( 0.80) as the third activator produces materials which furnish the Ce-emission in the near ultra-violet, the same as the silicates which contain only Ce or Ce together with Gd. In those cases where a relatively low Ce-content is opted for, it appears that materials containing also Pb and Gd are more efficient¯than the materials which contain Ce only. If terbium (y 41.0) is chosen as the third activator, very efficiently luminescing materials are obtained, which have the characteristic green terbium emission. The use of dysprosium (zS 0.1) as the third activator produces materials having an-efficient white dysprosium emission (predominantly an emission band in the yellow and, furthermore, a band in the blue part of the spectrum. A first embodiment of a luminescent silicate according to the invention is therefore characterized in that the silicate has a composition defined by the formula Me3-p Pbp Ln2 Si6 O18, wherein 0.03#p#0.25. These materials, which only contain lead as the activator are, particularly with lead contents between 0.03 and 0.25, very efficient radiators having a relatively narrow emission band (half value width approximately 40 nm) with a maximum at approximately 302 nm. They can therefore be used to great advantage in the luminescent screen of low-pressure mercury vapour discharge lamps for photo-chemical purposes, for example for the generation of erythema. According to the invention, a second embodiment of a luminescent silicate is characterized in that the silicate has a composition defined by the formula Me3-p Pbp Ln2-r Gdr Si6 O18, wherein 0.01#p#0.50 and 0.50 Xrg 2.0. The lead and gadolinium-activated silicates emit in a particularly efficient manner the characteristic Gd-radiation, especially at relatively high Gd-contents (r between 0.50 and 2.0). These materials are used in the luminescent screen of low-pressure mercury vapout discharge lamps for photo-chemical purposes, particularly in such lamps for radiation purposes, for example the photo-therapy of skin diseases, such as psoriasis. A third embodiment of a luminescent silicate according to the invention is characterized in that O (r 42-x 0.05 x #0.50 and furthermore p=q=y=z=O. These-silicates, which are only activated by Ce and which may possibly contain Gd are used in the luminescent screen of low-pressure mercury vapour discharge lamps for special purposes, for example in photo-copying apparatus, because they luminesce very efficiently in a band in the near ultra-violet and blue portion of the spectrum, particularly when x is chosen between 0.05 and 0.50. A further advantageous embodiment of a luminescent silicate according to the invention is characterized in that 0.01#p#0.50 0.05#r#2-y 0.05-yX 0.75 and furthermore q=x=z=O. Very high luminous fluxes are obtained on activation of the silicates by Pb, Gd and Tb, particularly for Tbcontents between 0.05 and 0.75. These green luminescing silicates are used in the luminescent screen of low-pressure mercury vapour discharge lamps for special purposes, for example for electro-photography, or in combination with a red and a blue luminescing material in such lamps for general lighting purposes. Another embodiment of a luminescent silicate according to the invention is characterized in that 0.01#p#0.50 0.05#r#2-z 0.0053 z4 0.08 q=x=y=O. The silicates activated by Pb, Gd and Dy are efficient, substantially white-light emitting materials, particularly with Dy-contents of 0.005 to 0.08. A luminescent screen provided with such a material can be used with great advantage in low-pressure mercury vapour discharge lamps for general lighting purposes. A still further embodiment of a luminescent silicate according to the invention is characterized in that 0.01# # p # 0.50 0.05#r# 2 0.005#q#0.15 x=y=Z=O. Activation of the silicates by Pb, Gd and Mn, particularly with Mn-contents of 0.005 to 0.15 provides very efficient, green-emitting materials. The Mn2+-emission in these materials appears to be a relatively long-wave emission (emission maximum at 540 to 550 nm), which can be very advantageous for practical uses. Such a luminescent silicate can be used in the luminescent screen of low-pressure mercury vapour discharge lamps for special purposes, such as electro-photography. These silicates may also be used as the green component in low-pressure mercury vapour discharge lamps for general used lighting purposes. Some embodiments of the invention will now be described and further explained with reference to the accompanying drawing and a number of measurements. In the drawing: Figure 1 shows the spectral energy distribution of the emitted radiation of three luminescent silicates according to the invention and Figure 2 shows the emission spectrum of three further silicates according to the invention. In the Figures 1 and 2 the maximum of each emission spectrum is set at 100. Example 1. A mixture is made of 3.003 g CaCO3 1.784 g ""203 3.786 g SiO2 (5 mole 0A in excess) 0.723 g CeO2. 0 This mixture was heated for 0.75 hour at 1250 C in a weakly reducing atmosphere. After cooling and pulverizing, the fired product was heated again for 3 hours at 1350 C in a weakly reducing atmosphere. After cooling, the product obtained was pulverized and mixed with 0.15 % by weight of NH4F and was then fired for one hour at 1350 C in a weakly reducing atmosphere. The product thus obtained was a luminescent, Ce-activated silicate having a composition defined by the formula Ca3 Y1.58 Ce0.42 Si6 O18 with a triclinic crystal structure. The use of a slight excess of Si02 and a very small quantity of NH4F, as indicated above, promotes the reaction. On excitation by the shortwave ultra-violet radiation from a low-pressure mercury vapour discharge lamp (predominantly 254 nm), the silicate luminesced efficiently (quantum efficiency approximately 53%) in a band having a maximum (- max) at 395 nm and a half value width (#¸) of approximately 70 nm. The peak height P of the emission band was 31% of the peak height of the known, lead-activated barium disilicate BaSi2O5-Pb used as a standard in this measurement. The emission spectrum of the silicate is shown in Figure 1 by means of curve 1. In this Figure the wavelength # (in nm) is plotted on the horizontal axis and the emitted radiation energy E in arbitrary units on the vertical axis. A large number of Ce-activated silicates were prepared in a similar manner to that described in Example 1. The following Table I shows for these silicates the formulae and measurements of P (in % of the above-mentioned standard) and of #max and #¸. TABLE I Example Formula (B) max t 2 (nm) (nm) 1 Ca 1.58 Ce0.42 Si6 018 31 395 70 2 Ca3 Y1.9 Ce0.1 Si6 O18 15 400 60 3 Ca3 Y1.8 Ce0.2 Si6 018 25 395 60 4 Ca3 Y1.7 Ce0.3 Si6 O18 26 400 60 5 Ca3 Y1.5 Ce0.5 Si6 O18 27 395 70 6 Sr3 Y1.9 Ce0.1 Si6 O18 20 385 60 7 Sr3 Y1.6 Ce0.4 Si6 018 23 390 70 5 1.0 0.4 @ @@ 8 Sr3 Gd1.9 Ce0.1 Si6 O18 17 385 60 9 Sr3 La1.9 Ce0.1 Si6 O18 19 380 55 10 Sr3 La0.9 CdCe0.1 Si6 O18 11 380 55 11 Sr2.9 Pb0.1 La0.9 GdCe0.1 Si6 O18 16 380 60 12 Ca3 Gd1.9 Ce0.1 Si6 018 20 390 55 13 Ca3 La1.9 Ce0.1 Si6 O18 17 390 60 14 Ca2.9 Pb0.1 La0.9 CdCe0.1 Si6 O18 17 390 70 Example 15. A mixture was made of 1.451 g CaCO 0.906 g Gd2O3 0.815 g La2O3 1.803 g SiO2 0.112 g PbO. This mixture was heated for 3 hours in air at a temperature of 13500C. After cooling and pulverizing, the product obtained was mixed with 0.5 by weight of NHCl and was then fire for 1 hour in air at a temperature of 125000. After cooling and pulverizing, the product was ready for use. It consisted of a luminescent silicate having a-tom-. position defined by the formula Ca2 9 Pb0.1 LaGd Si6 0 and had a triclinic crystal structure. The quantum efficiency of this silicate at 254 nm-excitation was approximately 59%. Figure 1 (curve 2) shows the emission spectrum of this silicate, this spectrum consisting of some very closely spaced lines (maximum at 313 nm, half value width of the emission band approximately 3 nm). Measured relative to the peak height of the known, Bi-activated gadolinium lanthanum metaborate Gd0.5 La0.487 Bi0.013B3O6 the emission peak height PH is 69%. A number of silicates activated by lead and gadolinium were prepared in a similar manner as described in the above example. The formulae of these materials, which all have the same emission spectrum, and the results of peak height PH measurements (relative to the abovementioned standard) are shown in Table II. TABLE II Example Formula PH (%) 15 Ca2.9 Pb0.1 La Gd Si6 018 69 16 Ca2.97Pb0.03La Gd Si6 018 57 17 2.8 Pb0.2 La Gd Si6 018 55 18 Sr2.97Pb0.03Y Gd Si6 O18 55 19 Sr2.9 Pb0.1 Y Gd Si6 O18 64 20 Sr2 8 Pb0.2 Y Gd Si6 018 53 21 Sr2.9 Pb0.1 La Gd Si6 O18 60 22 Sr2.9 Pb0.1 Gd2 Si6 O18 61 23 Ca2 9 Pb@ @ Y Gd Si6 018 31 Examples 24 to 28. Some silicates which were activated by Pb alone, were prepared in a similar manner to that described in Example 15. The formulae of these materials as well as the results of the peak height P measurements (relative to the standard mentioned in Example 1, that is the Pb-activated barium disilicate , the position of the emission maximum # max and half value width of the emission band #¸ are shown in Table III. TABLE III Example Formula P max max 2 (nm) (nm) 24 Ca2.9 Pb0.1 Y2 Si6 O18 61 307 38 25 x) Ca2.9 Pb0.1 La2 Si6 O18 69 303 42 26 Ca1.45 Sr1.45 Pb0.1Y2 Si6 O18 38 304 37 27 Sr2.9 Pb0.1 Y2 Si6 O18 56 302 42 28 Sr2.9 Pb0.1 La2 Si6 O18 71 302 40 x) The emission spectrum of this material (at 254 nmexcitation) is shown as curve 3 in Figure 1. Examples 29 to 38. Silicates, activated by Pb, Gd and Tb (Examples 29 to 33), by Pb, Gd and Dy (Examples 34 to 36) and by Pb, Gd and Mn (Examples 37 and 38) were prepared in a similar manner to that described in Example 15. Table IV shows the formulae of these silicates- as well as the results of the emission band peak height measurements (254 nm-excitation) positions of the emission maximum #max and half value width of the emission band #¸. The peak height P1 is given for the Tbactivated materials in % of the peak height of the known, Tb-activated cerium magnesium aluminate Ce0.67Tb0.33MgAl11O19 for the Dy-activated materials the peak height P2 is shown in fo of the peak height of the known Dy-activated yttrium vanadate YVO4-Gd; for the Mn-activated materials the peak height P3 is shown in % of the peak height of the known Mn-activated zinc silicate Zn2Sio4-Mn (willemite). TABLE IV Example Formula P1 P2 P3 #max #¸ (%) (%) (%) (nm) (nm) 29 Sr2.9 Pb0.1Gd1.98Tb0.02Si6O18 32 - - 543 12 30 a) Sr2.9Pb0.1Gd1.7Tb0.3 Si6O18 82 - - 543 12 31 Sr2.9Pb0.1Gd1.4Tb0.6Si6O18 73 - - 543 12 32 Sr2.9Pb0.1Y0.7GdTb0.3Si6O18 78 - - 543 12 33 Sr2.9Pb0.1La0.7GdTb0.3Si6O18 71 - - 543 12 34 Sr2.9Pb0.1Gd1.99Dy0.01Si6O18 - 18 - 573 20 35 b) Sr2.9Pb0.1Gd1.98Dy0.01Si6O18 - 20 - 573 20 36 Sr2.9Pb0.1Gd1.94Dy0.06Si6O18 - 15 - 573 20 37 c) Sr2.875Pb0.1Mn0.025Gd2Si6O18 - - 32 550 70 38 Sr2.8Pb0.1Mn0.1Gd2Si6O18 - - 17 550 70 a) The emission spectrum of this material is shown as curve 4 in Figure 2. b) The emission spectrum of this material is shown as curve 5 in Figure 2. c) The emission spectrum of this material is shown as curve 6 in Figure 2.

Claims: CLAIMS: 1. A luminescent silicate of an alkaline earth metal together with yttrium and/or lanthanum characterized in that the silicate has a composition defined by the formula Me3-p-q Pbb Mnq Ln2-r-x-y-z Gdr Cex Tby Dyz Si6 O18, wherein Me represents strontium and/or calcium and Ln yttrium and/or lanthanum, wherein, if q=r=z=y=z=0, it holds that 0.01#p#0.50, wherein, if p=q=y=z=O, it holds that 0.01#x#0.80 and 0#r#2-x, wherein, if q=x=y=z=O, it holds that 0.01#p#0.50 and 0.05g rX 2.0, and wherein otherwise it holds that 0.01#p#0.50 0.05#r#2-x-y-z 0#q#0.30 0#x#0.80 0#y#1.0 0#z#0.10 0.005#q+x+y+z. 2. A luminescent silicate as claimed in Claim 1, characterized in that the silicate has a composition defined by the formula Me3-p Pbp Ln2 Si6 018, wherein 0.03#p#0.25. 3. A luminescent silicate as claimed in Claim 1, characterized in that the silicate has a composition defined by the formula Me3-p Pbp Ln2-r Gdr Si6 O18, wherein 0.01#p#0.50 and 0.50#r#2.0. 4. A luminescent silicate as claimed in Claim 1, characterized in that 0 # r 2-x 0.05#x#0.50 and furthermore p=q=y=z=O. 5. A luminescent silicate as claimed in Claim 1, characterized in that 0.01#p#0.50 0.05#r#2-y 0.05#y#0.75 and furthermore q=x=z=O. 6. A luminescent silicate as claimed in Claim 1, characterized in that 0.01#p#0.50 0.05#r#2-z 0.005#z#0.08 q=x=y=0. 7. A luminescent silicate as claimed in Claim 1, characterized in that 0.01#p#0.50 0.05#r#2 0.005#q#0.15 x=y=z=O. 8. A luminescent screen comprising a luminescent silicate as claimed in Claims 1, 2, 3, 4, 5, 6 or 7. 9. A low pressure mercury vapour discharge lamp comprising a luminescent screen as claimed in Claim 8.

Inventors: KONIJNENDIJK, WILLEM LEENDERT, LOOYE, BOB, VERLIJSDONK, JOHANNUS GODEFRIDUS
Applicants: N.V. PHILIPS' GLOEILAMPENFABRIEKEN
Application year: 1980
Main classification: C09K11
IPC codes: C09K11, H01J61