HIGH-FREQUENCY CONDUCTOR HAVING IMPROVED CONDUCTIVITY

Abstract

A high-frequency conductor having improved conductivity comprises at least one electrically conductive base material. The ratio of the outer and inner surfaces of the base material permeable by a current to the total volume of the base material is increased by a) dividing the base material perpendicularly to the direction of current into at least two segments, which are spaced from each other by an electrically conductive intermediate piece and connected both electrically and mechanically to each other, and/or b) topographical structures in or on the surface of the base material and/or e) inner porosity of at least a portion of the base material compared to a design of the base material in which the respective feature was omitted. It was found that, as a result of these measures concerning the design, it is possible to physically arrange the same amount abase material so that a larger fraction of the base material is located at a distance of no more than skin depth from an outer or inner surface and is thus involved in current transport. As a result, a lesser fraction remains unused as a function of the skin effect.

Description

The invention relates to a high-frequency conductor having improved conductivity.

PRIOR ART

Direct current entirely permeates an electric conductor through which the current is conducted. Alternating current penetrates into the conductor only to a material- and frequency-dependent skin depth since the alternating magnetic field generated by the current, due to Lenz's law, induces a countervoltage in the conductor interior which pushes the current to the edge of the conductor. As a result, current transport is possible only in the edge region of the conductor cross-section to skin depth. The remaining conductor cross-section does not contribute to current transport. It is known to increase the conductor to reduce the electric resistance of the conductor, so that the edge region carrying the current also becomes larger. The drawback is that a small gain in conductivity is achieved in exchange for a large additional volume of conductor material, which due to the skin effect is not involved in current transport. The best-conducting metals are precious metals, which are thus very valuable.

PROBLEM AND SOLUTION

It is therefore the object of the invention to provide a high-frequency conductor that has improved conductivity, yet lower material costs.

This object is achieved according to the invention by a high-frequency conductor according to the main claim and by a production method according to the additional independent claim. Further advantageous embodiments will be apparent from the dependent claims.

SUBJECT MATTER OF THE INVENTION

Within the scope of the invention, a high-frequency conductor was developed which comprises at least one electrically conductive base material.

According to the invention, the ratio of the outer and inner surfaces of the base material permeable by a current to the total volume of the base material is increased by

• a) dividing the base material perpendicularly to the direction of current into at least two segments, which are spaced from each other by an electrically conductive intermediate piece and connected both electrically and mechanically to each other, and/or
• b) topographical structures in or on the surface of the base material and/or
• c) inner porosity of at least a portion of the base materialcompared to a design of the base material in which the respective feature was omitted,

It was found that, as a result of these measures concerning the design, it is possible to physically arrange the same amount of base material so that a larger fraction of the base material is located at a distance of no more than skin depth from an outer or inner surface and is thus involved in current transport, As a result, a lesser fraction remains unused as a function of the skin effect.

If the base material is segmented, advantageously at least one segment in every direction located perpendicularly on the direction of current has an extension between twice the skin depth of the base material at the maximum operating frequency and 2.5 times the skin depth of the base material at the lowest operating frequency. A lesser extension reduces conductivity, and a considerably higher extension only causes higher material costs, but no further gain in conductivity.

The intermediate piece is advantageously made of as material that is attacked by an etchant, against which the base material is resistant. The high-frequency conductor is then particularly easy to produce by growing alternating layers of the base material and of the material of the intermediate piece onto the substrate, and subsequently applying the etchant. The layers made of the material of the intermediate piece are then attacked simultaneously from two sides. A rest remains in the center between two areas of attack, the width of the rest being dependent on the etching duration and the etching rate. No complicated sequence of lithography steps is necessary.

The only requirements in regard to the intermediate piece are that the same has metallic conductivity and that it is mechanically stable. If the high-frequency conductor is applied to a semiconductor, there is a group of particularly suitable conductive materials available for every semiconductor, which form a Schottky contact with the semiconductor, for example.

The material of the intermediate piece is advantageously a metal from group 3A or 4A or a transition metal, or it contains at least one such metal as an alloying element. Particularly advantageously, the material of the intermediate piece belongs to the group (Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn), or it contains at least one metal from this group as an alloying element. These materials combine acceptable conductivity with good etchability, in particular when using wet-chemical etchants. However, when a production method is used in which this is not a factor, the material of the intermediate piece may also be a precious metal, for example. and in particular it may be identical to the base material.

If the base material is topographically structured, advantageously at least 30%, preferably at least 50%, and most particularly preferably at least 80% of the topographical structures in every direction located perpendicularly to the direction of current have an extension between twice the skin depth of the base material at the maximum operating frequency and 2.5 times the skin depth of the base material at the lowest operating frequency. The structures are then substantially completely permeated by the current.

If the base material is porous, the smallest distance between at least 30%, preferably at least 50%, and most particularly preferably at least 80% of the pores and the closest neighbors thereof is advantageously between twice the skin depth of the base material at the maximum operating frequency and 2.5 times the skin depth of the base material at the lowest operating frequency. The regions between the pores are then substantially completely permeated by the current, and only small amounts of base material that do not contribute to current transport remain.

The base material is advantageously carbon or a precious metal or semi-precious metal, or it contains at least one material from this group as an alloying element. In a particularly advantageous embodiment of the invention, the base material belongs to the group (Ru, Rh, Pd, Ag, Os, Ir, Pt, Au), or it contains at least one metal from this group as an alloying element. Carbon and these precious metals not only offer the best electrical conductivity, but are also resistant against environmental influences and against wet-chemical etchants, which may be used to produce intermediate pieces.

In a particularly advantageous embodiment of the invention, the high-frequency conductor is designed as a control electrode of a transistor, It may in particular be designed as the gate electrode of a field effect transistor. In the case of a field effect transistor, the important factor, in the interest of a preferably high switching frequency and edge steepness for the switching process, is to be able to apply a charge to the gate electrode as quickly as possible or, conversely, to be able to dissipate a charge from the same as quickly as possible.

As a gate electrode, the high-frequency conductor is advantageously coupled to the semiconducting gate of the field effect transistor via an electrically conducting intermediate piece, which defines the gate length, The shorter the gate length, the greater is the maximal switching frequency of the transistor.

In a further particularly advantageous embodiment of the invention, the high-frequency conductor is designed as a collector electrode or drain electrode of a photodetector. In particular in a photodetector according to the metal-semiconductor-metal (MSM) principle, quantum efficiency improves as the electrical resistance of the collector and drain electrodes decreases.

Based on the above, the invention also relates to a method for producing a high-frequency conductor according to the invention. To this end, alternating layers of the base material of the intermediate piece and of the base material are grown onto a substrate. The layer stack is subsequently exposed to an etchant, which isotropically etches the material of the intermediate piece, yet at the same time does not attack the substrate or the base material. The combination of the etching rate with the etching duration allows the width of the intermediate piece that remains after the etching process to be set,

Advantageously a dilutable etchant is selected. The etching rate can then be set by way of the degree of dilution. The etchant can be an acid or a base, for example. The dilution can be, but does not have to be, carried out with water. It is also possible, for example, to use other solvents for dilution.

SPECIFIC DESCRIPTION

The subject matter of the invention will be described hereafter based on figures, without thereby limiting the subject matter of the invention. In the drawings:

FIG. 1: shows an exemplary embodiment of the high-frequency conductor according to the invention;

FIG. 2: shows the frequency response of the achievable current density and a comparison to the prior art;

FIG. 3: shows an exemplary embodiment of the production method according to the invention;

FIG. 4: shows a scanning electron microscope image of the high-frequency conductor according to the invention and a comparison to the prior art; and

FIG. 5: shows a frequency response of the short circuit current gain of a transistor with the high-frequency conductor according to the invention as the gate, and a transistor comprising a gate according to the prior art.

FIG. 1 a shows a sectional drawing of an exemplary embodiment of the high-frequency conductor 1 according to the invention. The high-frequency conductor 1 is coupled via an intermediate piece 2 made of nickel, which defines the gate length, to an AlGaN/GaN heterostructure 3 as the semiconducting gate of a field effect transistor. This heterostructure is located on a sapphire substrate. The substrate as well as the source and drain regions of the transistor, including contacting, are not shown for the sake of clarity. The base material, which is gold, of the high-frequency conductor 1 is divided into two segments 1a and 1b, which are electrically and mechanically connected to each other by an intermediate piece 1c made of nickel. The current, which supplies a charge to the gate or dissipates the charge from the same again, flows perpendicularly to the drawing plane. Due to the skin effect, only the hatched fractions of the two segments 1a and 1b near the surface contribute to current transport through the high-frequency conductor 1. The current transport through the more poorly conducting intermediate pieces 1c and 2 is disregarded in FIG. 1 for the sake of clarity.

For comparison, FIG. 1b shows a sectional drawing of a high-frequency conductor 1 according to the prior art, which contains the same amount of base material as the exemplary embodiment according to FIG. 1a. Here, the division of the base material into two segments has been omitted. Consequently, the lower edge of segment I a and the upper edge of segment 1b are not regions near the surface which contribute to current transport. As a result, only a considerably smaller portion of the valuable base material is used for current transport.

FIG. 2 shows a log-log plot of the frequency response of the current density j achievable in the high-frequency conductor against the frequency f for the high-frequency conductor according to FIG. 1a (solid line) and FIG. 1b (dotted line). For frequencies starting at approximately 2*10¹⁰ Hz, a considerable gain in current density is apparent with the same use of base material.

FIG. 3 shows an exemplary embodiment of the production method according to the invention, which was used to produce the high-frequency conductor shown in FIG. 1a. Initially, alternating layers of nickel and gold, each having a thickness of 200 nm, were grown onto a commercially available AlGaN/GaN heterostructure 3 that was grown onto a sapphire substrate (FIG. 3a). The heterostructure is composed of a 3 μm thick undoped Ga N buffer layer, on which a 30 nm thick AlGaN barrier is located. AlN accounts for 26% in the mole fraction of this barrier. After having been grown on, the layer stack is exposed to hydrochloric acid diluted with water (HCl:H₂) 1:100), which attacked the nickel layers both from the right and the left (FIG. 3b). After etching, the layer stack was rinsed for 10 minutes in deionized water to stop further degradation of the nickel layers. AFM measurements showed that by the etching the mean (rms) roughness was not increased by the etching.

A nickel intermediate piece 2, which defines the gate length of the high electron mobility transistor (HEMT), remained directly on the heterostructure 3. The second nickel intermediate piece 1c connects the two segments 1a and 1b of the base material, which is gold.

FIG. 4 a shows a scanning electron microscope image of the high-frequency conductor according to the invention produced in this way, which corresponds to the pattern according to FIG. 1a, in a cross-sectional view (two-level T-gate). For comparison, FIG. 4b shows a cross-sectional view of a scanning electron microscope image of one example of the conventional T-gate structure (one-level T-gate) according to the prior art, which corresponds to the pattern according to FIG. 1b.

FIG, 5 shows the frequency response of the short circuit current gain g of a transistor comprising a conventional T-gate according to the prior art (FIG. 1b; thin dotted line) and of a transistor comprising a two-level T-gate according to the invention (FIG. 1a: thick solid line), each plotted against the frequency f. The two transistors are otherwise identically structured. The advantage of the transistor comprising the high-frequency conductor according to the invention as the gate is apparent at high frequencies. The high-frequency conductor according to the invention thus imparts a higher cut-off frequency f_max (maximum frequency transmitted without attenuation) to the transistor.

Claims

1. A high-frequency conductor, comprising at least one electrically conductive base material, wherein the ratio of the outer and inner surfaces of the base material permeable by a current to the total volume of the base material is increased bydividing the base material perpendicularly to the direction of current into at least two segments, which are spaced from each other by an electrically conductive intermediate piece and connected both electrically and mechanically to each other, compared to a design of the base material in which this division was omitted, wherein the intermediate piece is made of a material that is attached by an enchant, against which the base material is resistant.

2. The high-frequency conductor according to claim 1, wherein at least one segment in every direction located perpendicularly on the direction of current has an extension between twice the skin depth of the base material at the maximum operating frequency and 2.5 times the skin depth of the base material at the lowest operating frequency.

3. (canceled)

4. A high-frequency conductor according to claim 1, wherein the material of the intermediate piece is a metal from group 3A or 4A or a transition metal or comprises at least one such metal as an alloying element.

5. The high-frequency conductor according to claim 4, wherein the material of the intermediate piece belongs to the. group (Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn) or comprises at least one metal from this group as an alloying element.

6. (canceled)

7. (canceled)

8. A high-frequency conductor according to claim 1, wherein the base material is carbon or a precious metal or semi-precious metal. or that it comprises at least one material from this group as an alloying element.

9. A high-frequency conductor according to claim 1, wherein the base material belongs to the group (Ru, Rh, Pd, Ag, Os, Ir, Pt, Au) or comprises at least one metal from this group as an alloying element.

10. A high-frequency conductor according to claim 1, designed as a control electrode transistor.

11. The high-frequency conductor according to claim 10, designed as a gate electrode of a field effect transistor.

12. The high-frequency conductor according to claim 11, coupled to the semiconducting gate of the field effect transistor via an electrically conducting intermediate piece, which defines the gate length.

13. A high-frequency conductor according to claim 1, designed as a collector electrode or drain electrode of a photodetector.

14. A method for producing a high-frequency conductor according to claim 1, wherein alternating layers of the material of the intermediate piece and of the base material are grown onto a substrate, and the layer stack is subsequently exposed to an etchant, which isotropically etches the material of the intermediate piece, yet at the same time does not attack the substrate or the base material.

15. The method according to claim 14, wherein dilutable etchant is selected.