If the energy density of the pulse beam is 10 millijoules (mJ) per pulse, when this pulse beam is narrowed to a spot beam with the diameter of 0.1 mm, a peak output of about 1010 W/cm2 is gained.
Here, an Nd:YAG laser is used for the laser source 2, its oscillating wave length is 1.06 μm, the energy density per pulse is 10 mJ, repetition frequency is 20 Hz, and it is oscillated intermittently.
By this narrowing of the infrared laser beam, breakdown is caused in a gas in the air, which locally brings the gas into a high-density plasma state, whereby a flash light is generated locally. Also, together with the flash light, an impact noise is generated.
That is, when an infrared laser beam is collected by the condenser lens 11 at a visible-image formation scheduled point (drawing scheduled point) 13 in the air, a gas existing at the visible-image formation scheduled point 13 is locally brought into the plasma state, a flash light is generated at the visible-image formation scheduled point 13 in the air, and this visible-image formation scheduled point 13 is recognized as a light emitting point when visibly checked from a remote location.
Thus, as shown in FIG. 2, at a time t1, the scanning means 3 is controlled in the X direction so that an infrared laser beam is led to a visible-image formation scheduled point 13 a in the air, and the laser source 2 is oscillated immediately after that so as to have the gas at the visible-image formation scheduled point 13 a emit plasma light, and then, at a time t2, the scanning means 3 is controlled in the X direction so that the infrared laser beam is led to a visible-image formation scheduled point 13 b in the air and the laser source 2 is oscillated immediately after that so as to have the gas at the visible-image formation scheduled point 13 b emit plasma light and next, at a time t3, the scanning means 3 is controlled in the X direction so that the infrared laser beam is led to a visible-image formation scheduled point 13 c in the air and the laser source 2 is oscillated immediately after that so as to have the gas at the visible-image formation scheduled point 13 c emit plasma light.