CPC G01N 24/006 (2013.01) [C01B 32/26 (2017.08); C01B 32/28 (2017.08); C09K 11/65 (2013.01); C01P 2002/52 (2013.01); C01P 2006/60 (2013.01); C01P 2006/88 (2013.01)] | 16 Claims |
1. A method for producing a diamond with a high concentration of NV centers,
comprising:
providing a diamond blank:
wherein the diamond blank, when provided, comprises nitrogen atoms in a form of P1 centers; and/or
the diamond blank being of a yellow color when supplied; and/or
the diamond blank being of GIA colors “fancy yellow” or “fancy deep yellow” or “fancy light yellow” or “fancy intense yellow” when supplied; and/or
wherein the diamond blank, when provided, comprises nitrogen atoms together with hydrogen;
irradiating the diamond blank with particles:
wherein:
an energy of the particles is greater than 4 MeV;
an irradiation dose is between 5*1017 cm−2 and a*1019cm−2;
a temperature of the diamond blank during irradiation is greater than 600° C. and less than 1200° C.;
a radiation current of an electric current of the particles is adjusted such that an irradiation time to achieve the irradiation dose is at least 0.05 days;
the particles are electrons;
the temperature of the diamond blank is controlled by controlling a heating energy pulse height and/or a sensing factor and/or a temporal heating energy pulse spacing and/or a heating energy pulse width, whereby the control takes place in dependence on a temperature value;
the diamond blank is a synthetic HPHT diamond blank or a synthetic CVD diamond blank;
the temperature of the diamond blank during the irradiation is measured as a temperature value;
a total energy input to the diamond blank is composed of an energy from a heating device, a thermal energy derived via a thermal bleeder resistor, and a heating energy of the electron beam during the irradiation;
the diamond blank is heated with electrons during the irradiation;
the heating energy of the electron beam is determined by an energy of the electrons and an average beam current;
by controlling the total energy input by controlling at least one energy flow into the diamond blank during the irradiation and, if necessary, a total energy dissipation in such a way that a temperature probe placed in a vicinity of the diamond blank during the irradiation detects an average irradiation temperature of the diamond blank of greater than 600° C. and less 1200° C.;
the beam current of the electric current of the electrons of the electron beam is controlled;
a pulsed accelerator is used for the irradiation with the pulsed electron beam;
during irradiation a pulsation of the electron beam and thus also its heating energy is stabilized by a control system, such that a relevant controlled heating energy current, which heats the diamond blank during irradiation, is at least temporarily pulse-modulated in parts;
the heating energy is supplied pulsed or PWM-modulated or otherwise pulse-modulated by heating energy pulses;
the control is performed by adjusting the heating pulse width, the heating pulse spacing or a duty cycle of a pulse modulation of the heating pulses.
|