METHOD FOR TREATING A SURFACE OF A POLYMERIC PART BY MULTI-ENERGY IONS

Abstract

A treatment method for treating at least one surface of a solid polymer part wherein multi-energy ions X+ and X2+ are implanted simultaneously, where X is the atomic symbol selected from the list constituted by helium (He), nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), and xenon (Xe), and wherein the ratio RX, where RX=X+/X2+, with X+ and X2+ expressed as atomic percentages, is less than or equal to 100, for example less than 20. This results in very significant reductions in the surface resistivity of the parts treated in this way, the appearance of antistatic properties or of electrostatic charge dissipation properties. By way of example, the ions X+ and X2+ are supplied by an ECR source.

Description

The invention provides a treatment method for treating a polymer part by multi-charged and multi-energy ions belonging to the list constituted by helium (He), nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), and xenon (Xe).

By way of example, the invention finds application in the field of electronics, in which it is sought to prevent electrostatic charges being deposited, since that can destroy electronic components that are placed on a polymer substrate, or in the field of motor-vehicles, in particular so as to limit dust being deposited on a motor-vehicle instrument panel.

The majority of commercially available polymers do not conduct electric current. Their surface resistivity is in the range 10¹⁵Ω/□ [ohm per square] to 10¹⁷Ω/□.

However, electrical conduction may be desired for a number of reasons, including:

• • an antistatic effect: e.g. to avoid dust being deposited, plastic bags adhering together. A reduction in the surface resistivity that lasts for a few weeks or months may be sufficient;
  • dissipation of electrostatic charges: this is accomplished by means of dissipative materials and conductors that prevent electrical discharges and that dissipate the charges resulting from high speed movements;
  • electromagnetic shielding: materials with a very low volume resistivity (<1 ohm·cm [ohm-centimeter]) are required. Standards must be complied with in order to limit electromagnetic emissions from manufactured products.

Conductivity may be obtained by various routes:

• • non-permanent additives, such as fatty acid esters or quaternary amines. When incorporated into a polymer matrix, such substances migrate to the surface and react with the moisture in the air. They reduce the surface resistivity to approximately 10¹⁴Ω/□ by forming a moist film on the surface.
  • fillers that reduce surface resistivity and volume resistivity permanently. In particular, these are carbon blacks, carbon fibers, graphite, stainless steel fibers, aluminum flakes, and carbon nanotubes. Such fillers increase polymer manufacturing costs excessively when only superficial antistatic or electrostatic charge dissipation electrical properties are required.
  • intrinsically conductive polymers. These are both expensive and sensitive to conditions of use. Heat and moisture rapidly degrade their electrical properties.

Adhesion is a significant phenomenon with polymers that results in bits of paper, or dust adhering to a surface. Such adhesion results from the contribution of Van der Waals forces produced by the polarity of molecules located at the surface of the polymer and by the electrostatic forces induced by the very high surface resistivity.

In addition to problems with adhesion, polymer parts often need to function in chemical media of greater or lesser aggressivity, in ambient humidity, with ambient oxygen, at temperatures that are very low, or in contrast that are very high, etc., that may cause an increase in their electrically insulating nature by oxidation.

Certain polymers are filled with chemical agents for providing protection against UV or oxidation. Ejection of such chemical agents to the outside has the effect of accelerating surface oxidation, which in turn reinforces the insulating nature of the polymer.

The invention aims to reduce the above-mentioned disadvantages, in particular to substantially reduce the surface resistivity of a solid polymer part while retaining its bulk elastic properties and avoiding the use of chemical agents that are harmful to health.

Thus, the invention provides a method of treating at least one surface of a solid polymer part with helium ions, the method being characterized in that multi-energy ions X⁺ and X²⁺ are simultaneously implanted, where X belongs to the list constituted by helium (He), nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), and xenon (Xe), and where the ratio RX=X⁺/X²⁺, with X⁺ and X²⁺ being expressed as an atomic percentage, is less than or equal to 100, for example less than 20.

By way of example, the inventors have been able to establish that the simultaneous presence of He⁺ and He²⁺ ions can very significantly improve the antistatic surface properties of polymers compared with known treatments where only He⁺ or He²⁺ ions are implanted. They have been able to demonstrate that a significant improvement is observed for RHe less than or equal to 100, for example less than or equal to 20.

It should be noted that the invention can be used to reduce the surface resistivity of a solid polymer part and/or to eliminate dust adhesion, or even to reduce surface polarization by removing highly polarized chemical groups such as OH or COOH. Those functional groups may induce Van der Waals forces, which have the effect of bonding ambient chemical molecules to the polymer surface.

The invention can also be used to increase the chemical stability of the polymer, for example by creating a barrier to permeation. This can slow down the propagation of ambient oxygen within the polymer, and/or can retard the outward diffusion of agents contained in the polymer for protecting it against chemicals, and/or can inhibit leaching of toxic agents contained in the polymer towards the outside.

Advantageously, the invention can be used to dispense with adding chemical agents or fillers and to replace them with a physical method that is applicable to any type of polymer and that is less costly as regards material and energy consumption.

In the context of the present invention, the term “solid” means a polymer part produced by mechanical or physical transformation of a block of material, for example by extrusion, molding, or any other technique that is suitable for transforming a polymer block. Such transformations make it possible to obtain solid parts of various shapes, e.g. 3D parts, substantially 2D parts such as plates or profiled strips for example, and substantially 1D parts, such as wires.

Among the polymer parts that may advantageously be treated by the method of the present invention, mention may be made for example of polymer substrates for supporting electronic components so as to avoid electrostatic discharges that can destroy electronic components, or of motor-vehicle instrument panels so as to avoid dust being deposited.

In addition, the solid polymer part may be a portion of a part made of another material, e.g. it may be fitted to the part made of another material.

Examples of polymers that can advantageously be treated in accordance with the invention and that may be mentioned can be taken from the following materials:

• • polycarbonates (PC);
  • polyethylenes (PE);
  • polyethylenes terephthalates (PET);
  • polymethylacrylates (PMMA);
  • polypropylenes (PP);
  • polyamides (PA).

In an implementation, the multi-energy, multi-charged ions are produced simultaneously by an electron cyclotron resonance ion source (ECR).

Because of the method of the present invention, much greater depths can be treated, resulting in high chemical stability, resulting in very long-term preservation of surface electrical properties (antistatic, electrostatic charge dissipation).

The treatment times have been shown to be not long, having regard to industrial requirements.

Further, the method is low energy, low cost, and can be used in an industrial context without any environmental impact.

A polymer part is treated by simultaneously implanting multi-energy, multi-charged ions. These are in particular obtained by extracting single- and multi-charged ions created in the plasma chamber of an electron cyclotron resonance ion source (ECR source) using a single extraction voltage. Each ion produced by said source has an energy that is proportional to its charge state. This results in ions with the highest charge state, and thus the highest energy, being implanted in the polymer part at the greatest depths.

Implantation with an ECR source is rapid and inexpensive since it does not require a high extraction voltage for the ion source. In fact, in order to increase the implantation energy of an ion, it is economically preferable to increase its charge state rather than to increase its extraction voltage.

It should be noted that a conventional source such as a source that provides for the implantation of ions by plasma immersion or filament implanters cannot be used to obtain a beam that is adapted to the simultaneous implantation of multi-energy ions X⁺ and X²⁺ where the ratio RX is less than or equal to 100. With such sources, in contrast, it is generally 1000 or higher.

The inventors have been able to establish that this method can be used to surface treat a polymer part without altering its bulk elastic properties.

In accordance with one implementation of the present invention, the source is an electron cyclotron resonance source producing multi-energy ions that are implanted in the part at a temperature of less than 50° C.; the ions from the implantation beam are implanted simultaneously at a controlled depth depending on the extraction voltage of the source.

Without wishing to be bound by a particular scientific theory, in the method of the invention, as they pass through, the ions could be considered to excite the electrons of the polymer, causing covalent bonds to break and immediately recombine in order to result in a high density of covalent chemical bonds primarily constituted by carbon atoms by means of a mechanism known as cross-linking. Lighter elements such as hydrogen and oxygen are evacuated from the polymer during degassing. This densification into carbon-rich covalent bonds has the effects of increasing surface conductivity and of reducing or even completely removing the polar surface groups at the origin of the Van der Waals forces that are the source of adhesion. The cross-linking process is even more effective if the ion is light.

Helium is thus an advantageous projectile that is favored because:

• • it is very fast compared with the speed of the electrons of the covalent bonds, and it is thus very effective in exciting those same electrons, which as a consequence do not have time to modify their orbitals;
  • it penetrates to large depths of micrometer order;
  • it is not dangerous;
  • because it is a noble gas, it has no effect on the chemical composition of the polymer.

Other types of ions that are easy to use without any health risks may be envisaged, such as nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), or xenon (Xe).

Various preferred implementations of the method of the present invention are possible and may be combined together. A preferred implementation consists, for example, in combining:

• • the ratio RHe, where RHe=He⁺/He²⁺, where He⁺ and He²⁺ are expressed as an atomic percentage, is greater than or equal to 1;
  • the extraction voltage of the source for implantation of the multi-energy ions He⁺ and He²⁺ is in the range 10 kV [kilovolts] to 400 kV, for example greater than or equal to 20 kV and/or less than or equal to 100 kV;
  • the dose of multi-energy ions He⁺ and He²⁺ is in the range 5×10¹⁴ ions/cm² to 10¹⁸ ions/cm², for example greater than or equal to 10¹⁵ ions/cm² and/or less than or equal to 5×10¹² ions/cm², or even greater than or equal to 5×10¹⁵ ions/cm² and/or less than or equal to 10¹⁷ ions/cm²;
  • in a previous step, the variation as a function of doses of multi-energy ions He⁺ and He²⁺ in a characteristic property of the change in the surface of a solid polymer part is determined, for example the surface resistivity of the polymer of a polymer material that is representative of the part to be treated, in order to determine a range of ion doses in which the variation in the selected characteristic property is advantageous and varies in different ways in three consecutive zones of ion doses forming said ion dose range, with a change in the first zone that is substantially linear and reversible over a period of less than one month, a change in the second zone that is substantially linear and stable over a period of more than one month, and finally a change in the third zone that is constant and stable over a period of more than one month, and in which the dose of multi-energy He⁺ and He²⁺ ions in the third ion dose zone is selected for treatment of the solid polymer part; the term “reversible change” (first zone) means that the resistivity reduces, then rises to regain its original value. This phenomenon is due to the persistence of free radicals after implantation, which recombine with oxygen in the ambient air, thus causing an increase in the surface resistivity;
  • the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the speed of the surface treatment of the surface of the polymer part to be treated is in the range 0.5 cm²/s [square centimeter per second] to 1000 cm²/s, for example greater than or equal to 1 cm²/s and/or less than or equal to 100 cm²/s;
  • the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the implanted helium dose is in the range 5×10¹⁴ to 10¹⁸ ions/cm², for example greater than or equal to 5×10¹⁸ ions/cm² and/or less than or equal to 10¹⁷ ions/cm²;
  • the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the penetration depth of the helium on the surface of the treated polymer part is in the range 0.05 μm to 3 μm, for example greater than or equal to 0.1 μm and/or less than or equal to 2 μm;
  • the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the surface temperature of the polymer part during treatment is less than or equal to 100° C., for example less than or equal to 50° C.;
  • the polymer part is, for example, a profiled strip, and said part runs in a treatment device, for example at a speed in the range 5 m/min [meter per minute] to 100 m/min; by way of example, the polymer part is a profiled strip that runs longitudinally;
  • helium is implanted from the surface of the part to be treated by means of a plurality of multi-energy He⁺ and He²⁺ ion beams produced by a plurality of ion sources; by way of example, the ion sources are disposed in the direction of movement of the part to be treated; preferably, the sources are spaced such that the distance between two ion beams is sufficient to allow the part to cool between each successive ion implantation; said sources produce ion beams with a diameter that is adapted to the width of the tracks to be treated. By reducing the diameter of the beams to 5 mm [millimeter], for example, it is possible to place a highly effective differential vacuum system between the source and the treatment chamber, meaning that the polymers can be treated at 10⁻² mbar [millibar], while the vacuum in the source extraction system is 10⁻⁶ mbar;
  • the polymer of the part is selected from polycarbonates, polyethylenes, polyethylene terephthalates, polyamides, polymethylacrylates, and polypropylenes. The list is not exhaustive. Other generically cross-linkable types of polymer may be envisaged.

The invention also relates to a part wherein the thickness to which the helium is implanted is greater than or equal to 50 nm [nanometer], for example greater than or equal to 200 nm, and wherein the surface resistivity ρ is less than or equal to 10¹⁴Ω/□, for example less than or equal to 10⁹Ω/□, or even less than or equal to 10⁵Ω/□. Reference should be made to IEC standard 60093 for the measurement of surface resistivity.

The invention also provides the use of the above-mentioned treatment method for treating a solid polymer part selected from the list constituted by a polymer substrate for supporting an electronic component, a gasoline-tank part.

The present invention is described below by means of non-limiting implementations, in particular with reference to the accompanying drawings, in which:

FIG. 1 shows an example of the distribution of the helium implantation of the invention in a polycarbonate;

FIG. 2 shows the scales for various standards qualifying the electrostatic properties of a material;

FIG. 3 shows the variation in the surface resistivity of the surface of a polycarbonate sample treated in accordance with the invention, as a function of time, for a plurality of helium doses. The surface resistivity was measured using IEC standard 60093 employing an electrode constituted by a disk with diameter d surrounded by a ring with internal diameter D, where D is more than d;

FIG. 4 shows the variation in the surface resistivity of the surface of a polycarbonate sample treated in accordance with the invention, as a function of time, for three types of ions He, N, Ar in a plurality of doses. The surface resistivity was measured using IEC standard 60093; and

FIG. 5 shows the variation in surface resistivity of the surface of a polycarbonate sample treated in accordance with the invention, as a function of time, for a plurality of doses of nitrogen but using two beam movement velocities. The surface resistivity was measured using IEC standard 60093.

FIG. 1 shows a diagrammatic example of the implantation distribution of helium as a function of depth in accordance with the invention, in a polycarbonate. Curve 101 corresponds to the distribution of He⁺ and curve 102 to that of He²⁺. It can be estimated that for energies of 100 keV, He²⁺ covers a mean distance of approximately 800 nm for a mean ionization energy of 10 eV/Å [electron-volts per Angstrom]. For energies of 50 keV, He⁺ covers a mean distance of approximately 500 nm for a mean ionization energy of 4 eV/Å. The ionization energy of an ion is related to its cross-linking power. When (He⁺/He²⁺) is less than or equal to 100, it can be estimated that the maximum treated thickness is of the order of 1000 nm, i.e. 1 micrometer. These estimates agree with observations carried out by electron microscopy, which have demonstrated that for a beam extracted at 40 kV and a total dose of 5×10¹⁵ ions/cm² and (He⁺/He²⁺)=10, a cross-linked layer of approximately 750 nm to 850 nm is observed.

FIG. 2 shows the resistivity values qualifying the electrostatic properties of a material, in accordance with standard DOD HDBK 263. A polymer has insulating properties for surface resistivity values of more than 10¹⁴Ω/□ (ZONE I), and antistatic properties for values of surface resistivity in the range 10¹⁴Ω/□ to 10⁹Ω/□ (zone A). Electrostatic charge dissipation properties appear for values of surface resistivity in the range 10⁵Ω/□ to 10⁹Ω/□ (zone D) and conductive properties appear for values of less than 10⁵Ω/□ (zone C).

FIG. 3 shows the experimental change in surface resistivity of a polycarbonate as a function of time for different doses of helium equal to 10¹⁵ (curve 1), 2.5×10¹⁵ (curve 2), 5×10¹⁵ ions/cm² (curve 3), 2.5×10¹⁶ ions/cm² (curve 4), with He⁺/He²⁺=10; the extraction voltage is approximately 40 kV. The resistivity measurement was carried out in accordance with IEC standard 60093. The resistivity measurement technique employed did not allow resistivities of more than 10¹⁵Ω/□ to be measured, corresponding to zone N; it was saturated at 10¹⁵Ω/□. The abscissa corresponds to the time between the sample being treated and its surface resistivity being measured. The ordinate corresponds to the measurement of the surface resistivity, expressed in Ω/□. A first zone can be observed for doses of less than or equal to 10¹⁵ ions/cm², where the surface resistivity reduces over less than one month by approximately 3 orders of magnitude (from 1.5×10¹⁶Ω/□ to 5×10¹²Ω/□) before regaining its original value of about 1.5×10¹⁶Ω/□ (curve 1). In this zone, the antistatic properties are ephemeral, the free radicals still present recombining with oxygen in ambient air. In a second zone, the resistivity can be seen to decline as a function of dose: over the range 2.5×10¹⁵ ions/cm², 5×10¹⁵ ions/cm², 2.5×10¹⁶ ions/cm², the surface resistivity reduces from 10¹¹Ω/□ to 5×10⁹Ω/□ until it reaches a saturation plateau estimated to be at about 1.5×10⁸Ω/□. The antistatic properties (curves 2 and 3) are reinforced to become capable of dissipating electrostatic charges (curve 4). For these doses, the resistivities remained constant for more than 140 days. For doses of more than 2.5×10¹⁶ ions/cm², a third zone is reached where the change in resistivity saturates, as a function of dose, at about a value that is estimated to be 10⁸Ω/□ and remains stable over time for more than 140 days.

FIG. 4 shows the experimental change in surface resistivity of a polycarbonate (PC) as a function of time for three types of ions: He (curve 1), N (curve 2) and Ar (curve 3) for various doses equal to 10¹⁵ ions/cm², 5×10¹⁵ ions/cm², and 2.5×10¹⁶ ions/cm², with (He⁺/He²⁺)=10, (N⁺/N²⁺)=2 and (Ar⁺/Ar²⁺)=1.8. The beam diameter was 15 mm and the current was 0.225 mA; the extraction voltage was approximately 35 kV. The abscissa represents the dose in ions per unit surface area, expressed in 10¹⁵ ions/cm². The ordinate represents the surface resistivity, expressed in Ω/□. The resistivity measurement was carried out in accordance with IEC standard 60093. For the same dose, the heaviest ions were the most effective in reducing the surface resistivity; the PC treated with nitrogen had a surface resistivity at least 10 times lower than that of the PC treated with helium, the PC treated with argon had a surface resistivity at least ten times lower than that of the PC treated with helium. The inventors recommend using even heavier ions such as xenon to further reduce the surface resistivity of polycarbonate.

FIG. 5 shows the experimental change in the surface resistivity of a polycarbonate as a function of time for the same type of ions but at two different beam movement velocities—a movement speed of 80 mm/s (curve 1), a movement speed of 40 mm/s (curve 2)—for different doses equal to 10¹⁵ ions/cm², 5×10¹⁵ ions/cm², and 2.5×10¹⁶ ions/cm² (N⁺/N²⁺)=2. The beam diameter was 15 mm and the current was 0.150 mA; the extraction voltage was approximately 35 kV. The abscissa represents the dose in ions per unit surface area, expressed in 10¹⁵ ions/cm². The ordinate represents the surface resistivity, expressed in Ω/□. The resistivity measurement was carried out in accordance with IEC standard 60093. From these curves, it appears that reducing speed by a factor of 2 has the effect of reducing the surface resistivity of the PC by a factor of 10. Without wishing to be bound by any particular scientific theory, it could be considered that by reducing the speed of the beam, the surface temperature of the PC is increased. This temperature greatly increases recombination of free radicals between one another, at the same time favoring the formation of a dense, conductive film of amorphous carbon. Heating also has the effect of expelling residual gases produced by the scission/cross-linking mechanisms induced by ionic bombardment. The inventors deduced from this experiment that for any polymer treated with a beam with a known diameter and power, there exists a minimum beam movement speed causing a maximum reduction in surface resistivity of the polymer without risking degradation of the polymer under the effect of the heat produced. Thermal degradation of the polymer is indicated by substantial degassing followed by an increase in the pressure in the extraction system for the ECR source. This increase in pressure manifests itself in electrical breakdowns. The extraction system acts to extract ions from the plasma of the ECR source to form the beam. It is constituted by two electrodes, the first being earthed, and the second being brought to a high voltage of several tens of kV (kilovolts) under vacuum conditions of less than 5×10⁻⁶ mbar, preferably less than 2×10⁻⁶ mbar. Beyond these pressures, electric arcs are produced. This happens when thermal degradation of the polymer occurs. These rises in pressure should therefore be detected very early on by gradually reducing the beam movement speed and monitoring the change in pressure in the extraction system.

In order to determine this beam movement speed, the inventors recommend a test step that consists in gradually reducing the beam speed while retaining the other characteristics:

• • the beam characteristic: diameter, power, in other words intensity, and extraction voltage;
  • dynamic characteristics: amplitude of movement, rate of advance.

The polymer degrades thermally under the effect of heat when the pressure rise measured by a gauge located both in the extraction system and in the treatment chamber jumps by 10⁻⁵ mbar in a few seconds or even less. The tests must be stopped immediately to retain only the movement speed of the beam in the preceding test. This jump of 10⁻⁵ mbar in a few seconds or even less constitutes the signature of thermal degradation of the polymer.

Several characterization methods have allowed the advantages of the present invention to be highlighted.

In the examples below, the treatment of at least one surface of a solid polymer part by implantation of helium ions He⁺ and He²⁺ was carried out with multi-energy He⁺ and He²⁺ ions produced simultaneously by a ECR source. The treated polymers were the following in particular: polypropylene (PP), and polymethylacrylate (PMMA).

Comparative tests relating to the antistatic properties using small pieces of paper thrown onto the treated samples demonstrated that this appears for doses of more than 5×10¹⁵ ions/cm². For these doses, the pieces of paper detached and fell off when these samples were turned over, which did not happen for doses of less than 5×10¹⁵ ions/cm².

For polypropylene, a surface resistivity of 10¹⁴Ω/□ could be measured in accordance with IEC standard 60093 and for doses of 10¹⁵ ions/cm² and 5×10¹⁵ ions/cm². For a dose of 2×10¹⁶ ions/cm², it was possible to measure a resistivity of 5×10¹¹Ω/□, corresponding to the appearance of these antistatic properties.

In one implementation, it was estimated that the surface antistatic properties of a polymer were significantly improved from a dose of more than 5×10¹⁵ ions/cm², which represents a treatment speed of approximately 15 cm²/s for a helium beam constituted by 9 mA He⁺ ions and 1 mA He²⁺ ions.

The simultaneous implantation of helium ions may be carried out to various depths as a function of the requirements and shape of the part to be treated. These depths are in particular dependent on the implantation energies of the ions of an implantation beam; they may, for example, be from 0.1 μm to approximately 3 μm for a polymer. For applications where non-stick properties are desired, for example, a thickness of less than a micrometer would suffice, for example, further reducing the treatment period.

In one implementation, the conditions for implanting He⁺ and He²⁺ ions are selected such that the polymer part retains its bulk elastic properties by keeping the part at treatment temperatures of less than 50° C. This result may in particular be achieved for a beam with a diameter of 4 mm, delivering a total current of 60 microamps, with an extraction voltage of 40 kV, being moved at 40 mm/s over movement amplitudes of 100 mm. This beam has a power per unit surface area of 20 W/cm² [watt per square centimeter]. When using the same extraction voltage and the same power per unit surface area, and beams with a higher intensity while retaining the bulk elastic properties, a rule of thumb can be drawn up that consists in increasing the diameter of the beam, increasing the movement speed and increasing the amplitudes of the movements in a ratio corresponding to the square root of the desired current divided by 60 μA [microamps]. As an example, for a current of 6 milliamps (i.e. 100 times 60 microamps), the beam should have a diameter of 40 mm in order to keep the power per unit surface area at 20 W/cm². Under these conditions, the speed can be multiplied by a factor of 10 and the movement amplitudes by a factor of 10, which gives a speed of 40 cm/s and movement amplitudes of 1 m. The number of passes may also be multiplied by the same factor in order to have the same treatment dose expressed in ions/cm² in the end. With continuous running, the number of microaccelerators placed on the path of a belt, for example, may be multiplied by the same ratio.

It can also be seen that other surface properties are very significantly improved by means of a treatment in accordance with the invention; performance has been achieved that does not appear to have been attained with other techniques.

The invention is not limited to these types of implementations and should be interpreted in a non-limiting manner, encompassing treating any type of polymer.

Similarly, the method of the invention is not limited to the use of an ECR source, and even if it could be thought that other sources would be less advantageous, the method of the invention may be carried out with single-ion sources or with other multi-ion sources, as long as the sources are configured so as to allow simultaneous implantation of multi-energy ions belonging to the list constituted by helium (He), nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), and xenon (Xe).

Claims

1. A treatment method for treating at least one surface of a solid polymer part with ions, said method being characterized in that it comprises ionic bombardment with an ion beam constituted by multi-energy ions X+ and X2+, where X is the atomic symbol of the ion selected from the list comprising helium (He), nitrogen (N), oxygen (O), neon (Ne), argon (Ar), krypton (Kr), and xenon (Xe), wherein RX=X+/X2+, with X+and X2+, expressed as atomic percentages, being less than or equal to 100, for example less than 20, and wherein the movement speed of the beam is determined in a previous step in which the lowest movement speed of the beam is identified that does not cause thermal degradation of the polymer, as manifested by an increase in pressure of 10−5 mbar.

2. A treatment method according to claim 1, characterized in that the ions X+ and X2+ are produced simultaneously by an electron cyclotron resonance ion source (ECR).

3. A treatment method according to claim 1, characterized in that the ratio RX is greater than or equal to 1.

4. A treatment method according to claim 1, characterized in that the extraction voltage of the source allowing implantation of multi-energy ions X+ and X2+ is in the range 10 kV to 400 kV, for example greater than or equal to 20 kV and/or less than or equal to 100 kV.

5. A treatment method according to claim 1, characterized in that the dose of multi-energy ions X+ and X2+ is in the range 5×1014 ions/cm2 to 1018 ions/cm2, for example greater than or equal to 1015 ions/cm2 and/or less than or equal to 5×1017 ions/cm2 or even greater than or equal to 5×1015 ions/cm2 and/or less than or equal to 1017 ions/cm2.

6. A treatment method according to claim 1, characterized in that in a previous step, the variation as a function of the dose of multi-energy ions X+ and X2+ in a characteristic property of the change of the surface of a solid polymer part, for example the electrical resistivity of the surface, ρ, of a polymer material representative of that of the part to be treated, is determined in order to determine a range of ion doses wherein the variation in the selected characteristic property is advantageous and varies in different ways in three consecutive zones of ion doses forming said ion doses range, with a change in the first zone that is substantially linear and reversible over a period of less than one month, a change in the second zone that is substantially linear and stable over a period of more than one month, and finally a change in the third zone that is constant and stable over a period of more than one month, and wherein the dose of multi-energy ions X+ and X2+ in the third ion dose zone is selected to treat the solid polymer part.

7. A treatment method according to claim 1, characterized in that the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the areal speed of the surface of the polymer part to be treated is in the range 0.5 cm2/s to 1000 cm2/s, for example greater than or equal to 1 cm2/s and/or less than or equal to 100 cm2/s.

8. A treatment method according to claim 1, characterized in that the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the implanted ion dose is in the range 5×1014 ions/cm2 to 1018 ions/cm2, for example greater than or equal to 5×1015 ions/cm2 and/or less than or equal to 1017 ions/cm2.

9. A treatment method according to claim 1, characterized in that the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the penetration depth of the ion on the surface of the treated polymer part is in the range 0.05 μm to 3 μm, for example greater than or equal to 0.1 μm and/or less than or equal to 2 μm.

10. A treatment method according to claim 1, characterized in that the parameters of the source and of the movement of the surface of the polymer part to be treated are adjusted such that the temperature of the surface of the polymer part during treatment is less than or equal to 100° C., for example less than or equal to 50° C.

11. A treatment method according to claim 1, characterized in that the polymer part to be treated is an electronic part, for example, an extruded strip, and in that said part runs in a treatment device, for example at a speed in the range 5 m/min to 100 m/min;

12. A treatment method according to claim 1, characterized in that ion implantation from the surface of the polymer part to be treated is carried out by means of a plurality of multi-energy beams of X+ and X2+ ions produced by a plurality of ion sources.

13. A treatment method according to claim 1, characterized in that the type of polymer of the part is selected from polycarbonates (PC), polyethylenes (PE), polyethylene terephthalates (PET), polypropylenes (PP), polyamides (PA), polymethylacrylates (PMMA).

14. Use of the treatment method according to claim 1 for treating a solid polymer part selected from the list constituted by a substrate for supporting an electronic component and by a motor-vehicle instrument panel.