Patent Publication Number: US-2006007385-A1

Title: Optical attenuator and optical head device

Description:
TECHNICAL FIELD  
      The present invention relates to an optical attenuator and an optical head device, in particular to an optical head device to be used for recording or reproducing an information on an optical recording medium, and to an optical attenuator to be employed in the optical head device.  
     BACKGROUND ART  
      Recently, an optical recording medium capable of recording and/or reproducing information by irradiating with light has been widely used. As an example of such an optical recording medium, a CD-ROM for exclusive use for reproducing, having fine concavo-concave patterns corresponding to a recorded information formed on a substrate, is known.  
      Further, as another example of such an optical recording medium, an optical magnetic disk such as MO disk in which reproducing of an information is conducted by using magnetic Kerr effect, a phase-change type disk provided with a signal recording layer made of a phase change material, or a write-once optical disk such as a CD-R adapted to reproduce an information by detecting the difference of reflectivity at a recording mark which is formed in a signal recording layer made of an organic pigment material, have been known.  
      On the other hand, in order to record and/or reproduce various types of informations on the above various types of optical disks, various types of recording/reproducing devices employing optical head devices have been developed. In an optical head device for recording and/or reproducing an information on an optical recording medium such as CD-R, quantity of light converged on an optical recording medium by e.g. an objective lens needs to be large at a time of recording an information and needs to be small at a time of reproducing the information.  
      Heretofore, in order to satisfy this requirement, volume of emitted light from a laser diode has been changed by changing the injection current to the laser diode for emitting light. However, there has been such a problem that noise is increased or quantity of light becomes unstable when the injection current is reduced to reduce the emission quantity of light in some types of laser diode to be used.  
      A construction has been proposed which uses an optical attenuator in combination with the optical head device to irradiate an optical disk with a high quality laser light having little noise with low power so as to conduct a high quality recording and/or reproducing of an information with as low in noise as possible (for example, JP-A-202-260269).  
      Further, as an optical attenuator to be used for such an optical head device, one having a construction of combining a polarizing beam splitter (PBS) and a liquid crystal element has been known. The liquid crystal element changes the polarization state of incident laser light when a predetermined voltage is applied to the element, whereby the proportion of laser light transmitted through the polarizing beam splitter and incident into an optical recording medium is controlled depending on the polarization state.  
     DISCLOSURE OF THE INVENTION  
      There has been a problem that when the environmental temperature is changed, the ordinary refractive index and the extraordinary refractive index of the liquid crystal are changed and the attenuation amount of the optical attenuator using the liquid crystal element is changed.  
      Further, in an optical head device comprising the optical attenuator, when the polarization state such as the polarization direction of light incident into the liquid crystal element is changed, the volume of transmission light reaching an optical recording medium is changed. Therefore, it has been necessary to precisely control the polarization direction of light incident into the optical element, which has been causing an increase of cost for adjusting the polarization direction and reduction of yield.  
      The present invention provides an optical attenuator comprising a liquid crystal element which comprises a pair of transparent substrates having transparent electrodes formed on their respective surfaces facing to each other and a liquid crystal layer sandwiched between the transparent electrodes, whereby the direction of liquid crystal molecules in the liquid crystal layer is twisted spirally around the axis in the thickness direction of the liquid crystal layer, and at least one polarizing transmission element varying the transmittance depending upon the polarization state of the incident light, characterized in that the ordinary refractive index (n o ) and the extraordinary refractive index (n e ) of liquid crystal constituting the liquid crystal element, the angle (θ pt ) of the liquid crystal molecules close to a transparent substrate against the transparent substrate surface, the thickness (d) of the liquid crystal layer and the wavelength (λ) of incident light, are determined so that the value A satisfies a range of from 0.5 to 1.5 in the first conditional formula defined by the formula (1):  
             A   =       Δ   ⁢           ⁢     n   ·   d       λ             (   1   )             
 
 wherein 
 
Δ n=n   o   ·n   e   /√{square root over (n     o           2     ·cos     2     (θ     pt     )+n     e           2     ·sin     2     (θ     pt     ))}−   n   o  
 
      Further, the present invention provides the optical attenuator, wherein the angle (θ t ) between the two alignment directions of the respective liquid crystal molecules close to the pair of the transparent substrates, the quantity of light (P in ) incident into the optical attenuator and the quantity of light (P out ) output from the optical attenuator (provided that the light-reduction constant B is −60, and the value of the angle variable C is within a range of from 60 to 90), are determined so as to satisfy a second conditional formula defined by the formula (2):  
               θ   t     =           P   out     ·   B       P   in       +   C             (   2   )             
 
      Further, the present invention provides the attenuator, which has two such polarizing transmission elements, which are disposed on the light incident side and the light output side of the liquid crystal, respectively.  
      Further, the present invention provides the optical attenuator, wherein at least one of the two such polarizing transmission elements, is made to be a polarizing diffraction element whereby the diffraction efficiency varies depending upon the polarization direction of the incident light.  
      Further, the present invention provides the optical attenuator, wherein at least one of the two such polarizing transmission elements is made to be integral with the liquid crystal element.  
      Further, the present invention provides the optical attenuator, wherein the liquid crystal element is provided with nematic liquid crystal.  
      Further, the present invention provides the optical attenuator, wherein the transparent substrate is made of glass.  
      Further, the present invention provides an optical head device for reproducing and/or recording information, which comprises a light source, a light-converging means for converging light emitted from the light source on an optical recording medium, a photodetector for detecting a reflected light from the optical recording medium of the converged emission light, an optical attenuator to change the volume of the transmission light by an applied voltage, disposed in a light path between the light source and the optical recording medium or in a light path between the optical recording medium and the photodetector, and a voltage-controlling means to apply a voltage to the optical attenuator, characterized in that the optical attenuator is the optical attenuator.  
      Further, the present invention provides the optical head device, wherein the optical head device is an optical head device for carrying out reproducing and recording of information on an optical recording medium, wherein the ratio P 1 /P 2  is within a range of from 0.2 to 0.8, where P 1  is the quantity of light converged on the optical recording medium for reproducing information, and P 2  is the quantity of light converged for recording information 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       FIG. 1  is a side view showing an example of the optical attenuator of the present invention.  
       FIG. 2  is a view showing the alignment direction of liquid crystal unit and the transmission axis of a polarizing transmission element.  
       FIG. 3  is a graph showing the result of simulation experiment when the twist angle (θ t ) is 60°.  
       FIG. 4  is a graph showing the result of simulation experiment when the twist angle (θ t ) is 42°.  
       FIG. 5  is a graph showing the result of simulation experiment when the twist angle (θ t ) is 10°.  
       FIG. 6  is a graph showing the result of simulation experiment when the optical attenuation amount is 20±3%.  
       FIG. 7  is a graph showing the result of simulation experiment when the optical attenuation amount is 80±3%.  
       FIG. 8  is a graph showing the result of simulation experiment when the birefringency amount (Δn) of liquid crystal is 0.108.  
       FIG. 9  is a graph showing the result of simulation experiment when the birefringency amount (Δn) of liquid crystal is 0.136.  
       FIG. 10  is a schematic constructional view showing an example of the optical head device of the present invention.  
       FIG. 11  is a graph showing the relation between the voltage applied to the liquid crystal layer and the intensity of light transmitted through the optical attenuator with a parameter of angular error amount of polarization direction of incident light with respect to the liquid crystal unit.  
       FIG. 12  is a side view showing another example of the optical attenuator of the present invention.  
       FIG. 13  is a graph showing an example of the measurement of the relation between the directional error amount of polarization direction with respect to the optical attenuator and relative light intensity when the polarizing transmission element is disposed at the light-incident side. 
    
    
     BEST MODE FOR CARRYING OUT THE INVENTION  
       FIG. 1  shows an example of the optical attenuator of the present invention. Transparent substrates  101  and  102  made of e.g. a glass or a plastic are provided with transparent electrodes  103  and  104  made of e.g. ITO. Further, alignment films  105  and  106  made of e.g. polyimide are formed and subjected to an alignment treatment such as rubbing, and then, the two transparent substrates are disposed so that they oppose to each other with a gap of uniform spacing, and the periphery of the transparent substrates are bonded each other with e.g. an adhesive (not shown) to construct a cell structure. A liquid crystal is sealed in the cell to form a liquid crystal layer  107 . As the liquid crystal, e.g. a nematic liquid crystal may be used and a chiral compound may be added.  
      To the transparent electrode  103  and  104 , a voltage control unit  109  is connected which enable to apply a voltage from the outside, to constitute a liquid crystal unit  130 . An alignment treatment may be applied so that the liquid crystal molecules  108  are at an angle with respect to a polyimide surface at the interface between the polyimide and the liquid crystal layer. The angle is referred to as pretilt angle (θ pt ). The direction of liquid crystal molecules is twisted spirally around the axis in the thickness direction of the liquid crystal layer. The polarizing transmission element  110  is an element which changes the transmittance depending on a polarization state of incident light. In  FIG. 1 , light to be attenuated is incident into the liquid crystal unit  130  from the side of the transparent substrate  101 , output from the transparent substrate  102  and incident into the polarizing transmission element  110 . The polarizing transmission element  110  is preferably disposed at least behind the liquid crystal unit  130  in the traveling direction of light.  
       FIG. 2  shows the relation among alignment directions  202  and  203  of liquid crystal molecules at the respective interfaces between the liquid crystal layer and alignment films of the respective transparent substrates, and the transmission axis  201  of the polarizing transmission element. Light incident into the optical attenuator is a linearly polarized light polarized in an X axis direction. The angle between X axis and the alignment direction  202  of liquid crystal molecules at the interface between the liquid crystal layer and the alignment film ( 105  in  FIG. 1 ) on the transparent substrate in the light-input side of the liquid crystal unit  130 , is designated as pretwist angle (ep in  FIG. 2 ), and an angle between alignment directions  202  and  203  is designated as twist angle (θ t  in  FIG. 2 ). There is no limitation in the pretwist angle and the twist angle. However, the twist angle is preferably from 5 to 90° considering easiness of production. Further, the ordinary refractive index of the liquid crystal is designated as no, the extraordinary refractive index is designated as ne and the depth of the liquid crystal layer is designated as d. The wavelength of light to be attenuated is designated as λ.  
      When a voltage of at most a threshold voltage is applied to the liquid crystal layer, polarization of light transmitted through the liquid crystal unit is converted from a linear polarization to an ellipsoidal polarization in general. Then, a voltage is applied to drive liquid crystal molecules so that the direction of the liquid crystal molecules is in parallel with the direction of electric field. In this case, a linearly polarized light incident into the liquid crystal unit is transmitted through the liquid crystal unit as it is without changing the polarization state. By controlling the voltage applied to the liquid crystal unit, it is possible to change the polarization state of light transmitted through the liquid crystal unit and control the quantity of light transmitted through the polarizing transmission element after transmitted through the liquid crystal unit.  
      Here, the liquid crystal layer is considered as a group of N pieces of single-axis type birefringent plate in which the optical axis direction is twisted little by little, obtained by equally dividing the liquid crystal layer into N pieces in the direction of the thickness d. The phase difference r where the liquid crystal molecules are not twisted in the direction of the thickness of liquid crystal layer, namely, around a virtual axis in the thickness direction, is represented by the following formula:  
       Γ   =       2   ⁢     π   ·   Δ     ⁢           ⁢     n   ·   d       λ         
 
 wherein: 
 
Δ n=n   o   ·n   e   /√{square root over (n     o           2     ·cos     2     (θ     pt     )+n     e           2     ·sin     2     (θ     pt     ))}−   n   o  
 
      Provided that the twist is uniform in the direction of the thickness, the phase differences of the respective birefringent plates obtained by equally dividing the liquid crystal layer, is Γ/N. Where the polarization state of light incident into the liquid crystal unit and the polarization state of light transmitted through the liquid crystal unit are expressed by Stokes parameters and designated as S in  and S out  respectively, they are represented by the following expressions:  
         S   in     =     (         1           1           0           0         )         
         S   out     =     (         1             S   1               S   2               S   3           )         
 
      These formulae can be expressed as follows by using a Mueller&#39;s matrix: 
 
 S   out   R (θ p )· R (θ t   /N ) (N−1)   ·[W   (Γ/N)   ·R   (−θ     t     /N) ] (N−1)   ·W (Γ/ N )· R (−θ p )· S   in  
 
 wherein:  
         R   ⁡     (   φ   )       =     [         1       0       0       0           0         cos   ⁡     (     2   ⁢   φ     )             -     sin   ⁡     (     2   ⁢   φ     )             0           0         sin   ⁡     (     2   ⁢   φ     )             cos   ⁡     (     2   ⁢   φ     )           0           0       0       0       1         ]         
         W   ⁡     (   x   )       =     [         1       0       0       0           0       1       0       0           0       0         cos   ⁡     (   x   )             -     sin   ⁡     (   x   )                 0       0         sin   ⁡     (   x   )             cos   ⁡     (   x   )             ]         
 
      Provided that the polarizing transmission element is an ideal polarizer of single-axis type having a transmittance of 100% in X axis direction and 0% in Y axis direction, the transmittance P out  of the optical attenuator becomes as follows:  
         P   out     =         S   1     +   1     2         
 
 which becomes a function of n o , n e , d, θ t , θ p , θ pt  and λ. By calculating P out , a desired attenuation rate of the attenuator can be obtained. 
 
       FIGS. 3, 4  and  5  show simulation results. In each result, it is assumed that the birefringence amount of liquid crystal is (Δn)=0.1005 and the wavelength is (λ)=405 nm. Here, Δn is defined as birefringence amount. Twist angles (θ t ) are 60°, 42° and 10° in the results of  FIGS. 3, 4  and  5  respectively. The horizontal axis of each graph represents the thickness (d) of the liquid crystal layer, namely, the cell gap and the vertical axis represents the pretwist angle (θ p ). Each graph shows the relation between the thickness of liquid crystal layer and the pretwist angle where the optical attenuation amount becomes 50±3%. The distribution of pretwist angle (distribution of solution) with respect to the thickness of the liquid crystal layer where the optical attenuation amount becomes 50±3%, is changed depending on the twist angle (θ t ), and the distribution of solution becomes wide when the twist angle (θ t ) is 42° (in the case of  FIG. 4 ).  
      Particularly, the distribution of solution is wide at a liquid crystal layer thickness in the vicinity of 3.5 μm. If the distribution of solution is wide, it is possible to increase the tolerance for production-induced variation of parameter and to reduce the variation of optical attenuation amount due to a change of refractive index of liquid crystal caused by a change of environmental temperature, such being highly preferred.  
      The calculation is conducted at optical attenuation amounts of 20±3% and 80±3% in the same manner, and as a result, twist angles (θ t ) producing wide distribution of solution are present in the same manner and they are 60° and 24° for the respective optical attenuation amounts. The simulation results are shown in  FIGS. 6 and 7  respectively. A region of wide distribution of solution exists particularly at a liquid crystal layer thickness in the vicinity of 3.5 μm in the same manner as the case where the optical attenuation amount is 50%±3% (in the case of  FIG. 4 ).  
      Then, with respect to the cases where the birefringence amounts (Δn) of liquid crystal are 0.108 and 0.136, twist angles (θ t ) producing a wide distribution of solution for an optical attenuation amount of 50±3% were calculated and found that the twist angles (θ t ) became 42° in the same manner as the case of Δn=0.1005. The results are shown in  FIGS. 8 and 9 . The thickness of the liquid crystal layer producing particularly wide distribution of solution tends to decrease as Δn increases. As a result of repeated simulation, it was found that there is the following relation between Δn, d and λ:  
       A   =       Δ   ⁢           ⁢     n   ·   d       λ         
 
 where A is from 0.5 to 1.5, preferably from 0.75 to 0.95. In this case, the twist angle (θ t ) has the following relation with the transmittance (P out )  
         θ   t     =           P   out     ·   B       P   in       +   C         
 
 where B is −60 and C is from 60 to 90, preferably from 65 to 75. 
 
      By selecting the parameters (n o , n e , d, θ t , θ p , θ pt ) satisfying these conditions, and producing the liquid crystal unit, the tolerance for production-induced variation of parameters can be increased and the variation of optical attenuation amount when the refractive index of the liquid crystal is changed by the change of environment temperature, can be decreased.  
      Then, a case where the polarization direction of light incident into the optical attenuator of  FIG. 1  is changed is considered. For example,  FIG. 11  shows an example of intensity of light transmitted through the optical attenuator in response to the voltage applied to the liquid crystal layer provided that the incident light is linearly polarized light and polarized in X axis direction in  FIG. 2  and the polarization direction is rotated around Z axis. Three curves in  FIG. 11  show cases where the relative angular error between the polarization direction of linearly polarized incident light and X axis direction are 3°, 0° and −3° respectively. Thus by the relative angular error of the polarization direction, light intensity at a voltage in the vicinity of 0 V is changed.  
      Namely, in a case where the optical attenuator is used, for example, in a case where the intensity of light transmitted is increased (5 V) or decreased (0 V) by applying voltages of 5 V and 0V to the liquid crystal layer, the relative light intensities corresponding to these voltages are changed by the relative angular error between X axis direction and polarization direction of linearly polarized incident light. In other words, it becomes necessary to precisely control the polarization direction of linearly polarized incident light so as not to change the relative light intensities.  
       FIG. 12  shows another example of the optical attenuator of the present invention. Here, the same reference numerals as those used in  FIG. 1  indicate the same elements. By disposing the second polarizing transmission element  120  in the light-input side (in the side of the transparent  101 ) of the liquid crystal unit, polarization of light incident into the liquid crystal unit is stabilized by the second polarizing transmission element  120  even in a case where the polarization direction of light incident into the optical attenuator is changed, and the above-mentioned relative light intensity is not changed, such being highly preferred.  FIG. 13  shows an example of measurement of angular error of polarization direction of incident light into the optical attenuator and the relative light intensity in a case where the polarizing transmission element is disposed in the light-input side, as well as the result in a case where the polarizing transmission element is not disposed.  
      Further, as the polarizing transmission element, an absorption type polarizer produced by e.g. adding a pigment to a polymer followed by drawing, a wire grating or a polarizing beam splitter which changes substantial transmittance by changing the optical path by polarization direction, may be used. In particular, a polarizing diffraction element having different diffraction efficiencies depending on the polarization direction of the incident light, is preferred since it can be thin and it can be integrally formed with the liquid crystal unit to easily achieve miniaturization. The polarizing diffraction element can be produced by employing a liquid crystal, a high-molecular liquid crystal or a birefringent medium such as lithium niobate (LiNbO 3 ).  
      Further, it is more preferred that the liquid crystal unit and the polarizing transmission element is integrally formed since it enables to achieve miniaturization, light-weight, reduction of the number of parts and the like.  
      Further,  FIG. 10  shows an example of an optical head device including the optical attenuator thus produced. The optical attenuator of the present invention is constituted by the liquid crystal element  3 , and the polarizing transmission elements  4  and  12  which are disposed between the collimator lens  2  and quater-waveplate  8 . Light emitted from a laser diode  1  is converted to be a parallel light by the collimator lens  2 , transmitted through the polarizing transmission element  12  and transmitted through the liquid crystal element  3 . The liquid crystal element  3  can be applied with a voltage from the outside by means of a voltage control device  11 . The light transmitted through the liquid crystal element  3  is transmitted through the polarizing transmission element  4 . The polarizing transmission element  4  changes the quantity of light output to the optical recording medium depending on the polarization direction of incident light when the light incident into this element is output. The polarizing transmission element  4  may, for example, be a polarizing beam splitter, a prism, a diffraction grating including a wire grating, or a polarizing diffraction element. In the example of  FIG. 10 , a polarizing beam splitter is employed as the polarizing transmission element  4 , and a polarizing diffraction element is employed as the polarizing transmission element  12 . Further, the polarizing transmission elements  4  and  12  can be adhered to the liquid crystal element  3  to be integrally formed. The light transmitted through the polarizing transmission element  4  is transmitted through a quater-waveplate  8  and converged on the optical recording medium  7  by a converging lens  5  held by an actuator  6 .  
      Light reflected by the optical recording medium  7  travels reversely through the above optical path. In the case of  FIG. 10 , since a polarizing beam splitter is employed as the polarizing transmission element  4 , the light reversely traveling through the optical path is reflected by the polarizing transmission element  4  and converged by the converging lens  9  to reach the photodetector  10 . Here, by applying plural different voltages to the liquid crystal element  3 , (actually to transparent electrodes formed on the surfaces of the transparent substrates constituting the liquid crystal element), it is possible to change the polarization direction of the light transmitted through the liquid crystal element  3  and change the quantity of light converged on the optical recording medium after transmitted through the polarizing transmission element  4 .  
      The ratio P 1 /P 2  of the quantity of light P 1  converged on the optical recording medium for reproducing an information of the optical recording medium to the quantity of light P 2  converged for recording an information into the optical recording medium, is preferably within a range of from 0.2 to 0.8, more preferably within a range of from 0.3 to 0.6. If the ratio of quantity of light is within this range, recording of information is sufficiently possible by making the quantity of light 100% at a time of recording an information, and at a time of reproducing, by making the quantity of light to be within a range of from 20 to 80% (namely from 0.2 to 0.8), preferably within a range of from 30 to 60% (namely from 0.3 to 0.6), with respect to the quantity of light for recording, reproducing of information can be achieved without recording an information into the optical recording medium and with high S/N ratio, such being highly preferred.  
      Now, Examples are described as follows.  
      An optical attenuator having an optical attenuation ratio of 36.5% to be used for a wavelength of 405 nm was produced. The detail of the production is described as follows by using  FIGS. 1 and 2 . With respect to the liquid crystal unit, as shown in  FIG. 1 , on transparent substrates  101  and  102  of 1.0 mm thick and made of glass, transparent electrically conductive ITO films of 30 nm thick were formed by a sputtering method, and patterned by photolithography and wet etching methods to form transparent electrodes  103  and  104 . On the transparent electrodes  103  and  104  on the transparent substrate  101  and  102 , alignment films  105  and  106  of polyimide of about 50 nm thick were applied by a flexo printing method and baked. An alignment treatment by rubbing with a cloth was applied to the alignment films  105  and  106  of polyimide film. This alignment treatment was conducted so that the liquid crystal molecules  108  were twisted around the axis in the thickness direction of the liquid crystal layer  107 . An epoxy type sealing material (not shown) was printed on the transparent substrate  101  by a screen printing method. In the epoxy type sealing material (not shown), 3% (in mass ratio. Hereinafter the same definition is applied) of fiber spacers having a diameter of 3.6 μm for fixing the thickness of the liquid crystal layer, and 2% of plastic balls having a diameter of 4 μm and having a surface provided with an electrically conductive coating to obtain conductivity between the transparent substrates  101  and  102 , were contained. After the transparent substrates  101  and  102  were overlayed and aligned to each other, they were pressed to be bonded with a pressure of 6×10 4  N/m 2 , at a temperature of 170° C. to form a cell. Into the cell thus formed, a nematic liquid crystal was injected by a vacuum injection method to form a liquid crystal layer  107 , and the injection port was sealed with a UV adhesive agent (not shown) to form a liquid crystal element having an external dimension of 8 mm×10 mm. The liquid crystal element is adapted for application of voltage to the liquid crystal layer from the outside via the transparent electrodes  103  and  104 . The parameters of the liquid crystal element (liquid crystal unit of the optical attenuator) were made to be θ p =−10°, θ t =5°, Δn=0.1005 and d=3.6.  
      The liquid crystal element thus produced was integrated into an optical head device as shown in  FIG. 10 . The liquid crystal element  3  was disposed between a polarizing beam splitter being a polarizing transmission element  4  disposed in the optical head device and a polarizing diffraction element being a polarizing transmission element  12 . The liquid crystal element was controlled by output voltage from a voltage control device  11 . Light emitted from a laser diode  1  was transmitted through a collimator lens  2 , the polarizing transmission element  12 , the liquid crystal element  3 , the polarizing beam splitter as the polarizing transmission element  4  and quater-waveplate  8  in this order, and converged on an optical recording medium  7  after transmitted through a converging lens  5  held by an actuator  6 . The light converged was reflected by the optical recording medium  7 , transmitted through the converging lens  5  and quater-waveplate  8  in this order to have its polarization direction changed by 90°, and reflected by the polarizing beam splitter and introduced to a photodetector  10  by a converging lens  9 .  
      In this condition, the liquid crystal element  3  was applied with a voltage, a photodetector was disposed at the position of the optical recording medium  7  and the quantity of light converged was measured. As a result, it was found to be 37% (the quantity of light under application of a voltage of 10 V rms  (a rectangular alternating current of 1 kHz) is defined as 100%) under application of a voltage of 0.4 V rms  (a rectangular alternating current of 1 kHz) to the liquid crystal element, and the quantity of light converged on the optical recording medium  7  could be changed by the voltage applied to the liquid crystal. When an information recording to an optical recording medium is conducted by employing the optical head device, the liquid crystal element  3  is applied with a voltage of 10 V rms  (a rectangular alternating current of 1 kHz) to allow a large quantity of light to be converged on the optical recording medium  7 . When reproducing of an information from the optical recording medium  7  is conducted, the voltage applied to the liquid crystal element  3  is set to be 0.4 V rms  (a rectangular alternating current of 1 kHz) to attenuate the quantity of light converged on the optical recording medium  7  to be 37% without changing the output power of the laser diode  1 . Thus, reproduction of an information was carried out with low noise. Further, it was confirmed that variation of the optical attenuation amount was maintained to be on a low level under the environmental temperature changed from 10° C. to 60° C.  
     INDUSTRIAL APPLICABILITY  
      The present invention can provide an optical attenuator having a small variation of optical attenuation amount under the change of environmental temperature, or an optical attenuator having a small variation of optical attenuation amount in response to the change of polarization state of incident light such as polarization direction, and an optical head device comprising the above optical attenuator excellent in recording and reproducing properties of information.  
      Further, the optical attenuator can be used also as e.g. a variable attenuator to be used for optical communication system in the near-infrared wavelength region such as 1,550 nm wavelength region.  
      The entire disclosures of Japanese Patent Application No. 2003-061812 filed on Mar. 7, 2003 and Japanese Patent Application No. 2003-307130 filed on Aug. 29, 2003 including specifications, claims, drawings and summaries are incorporated herein by reference in their entireties.