High-frequency power supply device and ignition voltage selection method
When RF power is supplied from an RF generator to a load via a power supply unit, (a) the internal impedance of the RF generator is made lower than the characteristic impedance of the power supply unit, and (b) the load-end voltage is increased by selecting the electrical length L E of the power supply unit, which connects between the RF generator and the load to supply RF power, so that the electrical length L E has a predetermined relation with the fundamental wavelength λ of the RF AC. More specifically, the electrical length L E of the power supply unit is selected in such a way that, when the load end, which is the input end of the load, is in an open state, the electrical length L E is (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is {π−2·cos −1 (1/K)}/(4π)) with respect to the fundamental wavelength λ of the RF AC.
1. An RF power supplying device comprising:
an RF generator unit that converts a DC of a DC power supply to an RF AC through a switching operation; and
a power supply unit connected between an output end of said RF generator unit and a load end, which is an input end of a load, to supply the RF AC to the load, wherein
an internal impedance of said RF generator unit is lower than a characteristic impedance of said power supply, and
an electrical length (L E ) of said power supply unit when the load end is in an open state is a value selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to a fundamental wavelength λ of the RF AC.
2. The RF power supplying device according to claim 1 wherein,
said power supply unit is a feed cable that electrically connects between the output end of said RF generator unit and the load end of said load,
the internal impedance of said RF generator unit is lower than a characteristic impedance of said feed cable, and
an electrical length L E of a cable length of said feed cable when the load end of said load is in an open state is a length in electrical length selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC.
3. The RF power supplying device according to claim 1 wherein,
said power supply unit is a filter circuit that electrically connects between the output end of said RF generator unit and the load end of said load, the filter circuit being a series resonant circuit of a capacitor and a reactor,
the internal impedance of said RF generator unit is lower than the characteristic impedance of said filter circuit, and
an electrical length L E of said filter circuit when the load end is in an open state is an electrical length selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC.
4. The RF power supplying device according to claim 1 wherein,
said power supply unit is a series circuit that electrically connects between the output end of said RF generator unit and the load end of said load, the series circuit including a filter circuit and a feed cable, the filter circuit being a circuit of a capacitor and a reactor,
the internal impedance of said RF generator unit is lower than the characteristic impedance of said series circuit, and
an electrical length L E of said series circuit when the load end is in an open state is an electrical length selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC.
5. The RF power supplying device according to claim 1 wherein,
the constant k is {π−2·cos −1 (1/K)}/(4π) and is a constant defining a range of an electrical length L E that makes a load-end voltage (V z (z=L E )) the K times of an RF generator voltage V g .
6. An ignition voltage selection method that causes a plasma load to generate a plasma discharge at a load end that is an input end of the plasma load, the ignition voltage selection method performed when an RF generator unit supplies an RF AC to the plasma load via a power supply unit, the ignition voltage selection method comprising the steps of:
converting, by said RF generator unit, a DC of a DC power supply to an RF AC through a switching operation to make an internal impedance of said RF generator unit lower than a characteristic impedance of said power supply unit;
when said plasma load is in a non-discharge state, setting an electrical length L E of said power supply unit when the load end of the plasma load is in an open state to (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to a fundamental wavelength λ of the RF AC; and
selecting a voltage of the load end of said plasma load, determined by the electrical length L E , as an ignition voltage.
7. The ignition voltage selection method according to claim 6 wherein,
said power supply unit is a feed cable that electrically connects between an output end of said RF generator unit and the load end of said plasma load,
the internal impedance of said RF generator unit is lower than a characteristic impedance of said feed cable,
an electrical length L E of a cable length of said feed cable when the load end of said plasma load is in an open state is a length selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC, and
a voltage of the load end of said plasma load, determined by the cable length, is selected as the ignition voltage.
8. The ignition voltage selection method according to claim 6 wherein,
said power supply unit is a filter circuit that electrically connects between an output end of said RF generator unit and the load end of said plasma load, the filter circuit being a circuit of a capacitor and a reactor,
the internal impedance of said RF generator unit is lower than the characteristic impedance of said filter circuit,
values of the capacitor and the reactor of said filter circuit are adjusted so that an electrical length L E when the load end of said plasma load is in an open state is selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC, and
a voltage of the load end of said plasma load, determined by said filter circuit, is selected as the ignition voltage.
9. The ignition voltage selection method according to claim 6 wherein,
said power supply unit is a series circuit that electrically connects between an output end of said RF generator unit and the load end of said plasma load, the series circuit including a filter circuit and a feed cable, the filter circuit being a circuit of a capacitor and a reactor,
the internal impedance of said RF generator unit is lower than the characteristic impedance of said series circuit,
in said series circuit, a length of said feed cable and values of the capacitor and the reactor of said filter circuit are adjusted so that an electrical length L E when the load end of said plasma load is in an open state is selected as (2n−1)·(λ/4)−k·λ≦L E ≦(2n−1)·(λ/4)+k·λ (n is an integer, k is a constant in a range of 0 to λ/4) with respect to the fundamental wavelength λ of the RF AC, and
a voltage of the load end of said plasma load, determined by said series circuit, is selected as the ignition voltage.
10. The ignition voltage selection method according to claim 6 wherein,
the constant k is {π-2·cos −1 (1/K)}/(4π) and is a constant defining a range of an electrical length L E that makes a load-end voltage (V z (z=L E )) the K times of an RF generator voltage V g .