[0001] The present invention generally relates to a photocatalytic ignition system and particularly,
but not exclusively, to a photocatalytic ignition system that uses a photocatalyst
to ignite a mixture of a fuel gas and air. Aspects of the invention relate to an apparatus,
to a system, to an engine and to a vehicle.
[0002] In recent years, attention has been directed toward photocatalysts. When a photocatalyst
absorbs an amount of light energy equal to or exceeding a band gap energy, it develops
holes due to the excitation of valence electrons to the conduction band. It is believed
that the electrons and holes move to the surface of the catalyst and produce hydroxyl
radicals, super oxide anions, and other active species. The active species have a
very high oxidation strength and will readily oxidize and decompose organic substances.
The photocatalytic action of photocatalysts has been used for air cleaning, water
cleaning, anti-soiling, and anti-fogging (e.g.,
Ceramics, Akira Fujishima, 39, 2004, No. 7).
[0003] So long as a photocatalyst can absorb light, the photocatalytic reaction will proceed
according to the mechanism described above and clean solar energy can be used. Thus,
although a photocatalyst does not require a supply of heat energy or other external
energy in order to stimulate the catalytic reaction in the manner of conventional
technologies, it has been difficult to obtain a sufficient reaction rate with a photocatalyst.
It has been suggested that a reason a sufficient reaction rate cannot be obtained
is that the utilization efficiency of sunlight is small. Currently, titanium oxide
is the most commonly used photocatalytic material due to its lower cost and chemical
stability. However, the band gap energy of titanium oxide is 3.2 eV (which is high).
Thus, titanium oxide can only absorb ultraviolet light. The content of ultraviolet
light in sunlight is only approximately 3%. In fluorescent lamps for indoor use, the
fluorescent material converts ultraviolet light into visible light. Since many vehicles
use window glass that cuts ultraviolet rays, only visible light is actually available
for use inside such vehicles.
[0004] The content of visible light in sunlight is approximately 50%. If visible can be
used, then a faster reaction rate can be obtained. Ways of reducing the band gap energy
are being investigated to enable the use of visible light. Since the energies of the
conduction band and the valence band are determined by the orbitals of oxygen, the
band gap energy can be reduced by controlling one of the orbitals. Based on previous
observations, it is known that when an orbital of the metal atom is controlled, a
recombination center for electrons and holes is produced and the activity level of
the photocatalyst declines. Consequently, it is necessary to replace the oxygen with
an element whose valence band has a higher energy level than the valence band of oxygen.
[0005] Since the valence electron of a nitrogen atom has a higher energy than the valence
electron of an oxygen atom, the band gap energy can be decreased and visible like
can be utilized by using nitrogen. Proposals have been made for using an oxynitride
material (e.g., Japanese Laid-Open Patent Publication No.
2002-066333 and Japanese Laid-Open Patent Publication No.
2004-230306) or titanium oxide that has been doped with nitrogen using a NOx treatment or an
ammonia treatment (
What Is a Photocatalyst?, Shinri Sato, Kodansha, 2004).
[0006] Meanwhile, there are various research and development projects focusing on improving
the catalytic activity of the catalyst. For example, catalysts are being combined
with porous substances in order to increase the amount of reactant material that adheres
to a surface of the catalyst and such techniques as improving crystallinity and reducing
the particle size of powder are being used to enable electrons and holes produced
by photoexcitation to reach the catalyst surface without losing their activity level
(e.g., Japanese Laid-Open Patent Publication No.
2001-259436). Another idea is to provide a metal material in order to promote electric charge
separation (e.g., Japanese Laid-Open Patent Publication No.
9-262473).
[0007] Much research and development is being conducted in relation to applications of photocatalysts
and there are numerous reports of such applications as producing hydrogen by decomposing
water and removing stains by decomposing organic matter. There are also applications
in which a hydrophilic mesh sheet, particularly a hydrophilic mesh sheet having a
photocatalyst-containing layer provided as a hydrophilic layer, is installed inside
a greenhouse and used to adjust the temperature and/or humidity inside the greenhouse.
Water is allowed to flow down onto the hydrophilic mesh sheet and evaporate. The heat
of evaporation required to evaporate the water lowers the ambient temperature and
the vaporized moisture can be used to adjust the ambient humidity. (e.g., Japanese
Laid-Open Patent Publication No.
2005-013132)
[0008] More recently, the idea of using a photocatalyst to ignite an air fuel mixture was
proposed (e.g., Japanese Laid-Open Patent Publication No.
2006-307839) and, thus, a method of igniting an air fuel mixture using light became publicly
known. In the proposed method, light is focused in a space so as to form a thermal
plasma and ignite an air fuel mixture. Consequently, the method has the disadvantage
of a minimum ignition energy being high. It has been reported that the minimum ignition
energy can be lowered by using a target (e.g., Japanese Laid-Open Patent Publication
No.
58-133482 and Japanese Laid-Open Patent Publication No.
59-221523).
[0009] As described above, an air fuel mixture igniting system that uses a photocatalyst
brings the advantage of enabling the minimum ignition energy to be reduced because
the radicals necessary for igniting the air fuel mixture can be produced comparatively
readily at the surface of the photocatalyst. However, a highly effective photocatalytic
material has not been proposed and the ability of existing photocatalytic materials
to lower the minimum ignition energy is not sufficient. Consequently, a practical
photocatalytic ignition system has yet to be proposed.
[0010] It is an aim of the present invention to address this issue and to improve upon known
technology. Embodiments of the invention may provide an improved photocatalytic ignition
system that uses a photocatalyst to ignite a mixture of a fuel gas and air and that
can ignite a lean air fuel mixture with a much smaller amount of light energy than
previously proposed systems. Other aims and advantages of the invention will become
apparent from the following description, claims and drawings.
[0011] Aspects of the invention therefore provide an apparatus, a system, an engine and
a vehicle as claimed in the appended claims.
[0012] According to another aspect of the invention for which protection is sought there
is provided a photocatalytic ignition system comprising an ignition chamber configured
to receive an air fuel mixture, a photocatalyst arranged in the ignition chamber to
contact the air fuel mixture and a light source arranged to shine light on the photocatalyst,
the photocatalyst including a photocatalytic material having an oxygen absorbing and
a desorbing function.
[0013] In an embodiment, the photocatalytic material is at least one selected from a group
consisting of cerium oxide, titanium oxide and copper oxide.
[0014] In an embodiment, the photocatalytic material is cerium oxide with an average particle
size of 20 nm or smaller.
[0015] In an embodiment, the photocatalyst further includes a photothermal conversion material
that includes at least one transition metal compound selected from a group consisting
of transition metal sulfides, transition metal nitrides and oxides of transition metals
other than cerium, titanium and copper.
[0016] In an embodiment, the photothermal conversion material includes at least one of iron
and vanadium as a transition metal of the transition metal compound.
[0017] In an embodiment, the photocatalytic material is cerium oxide, the photothermal conversion
material is an oxide of iron, and the mole ratio of cerium to iron contained in the
photocatalyst lies in the range of 2/8 to 8/2.
[0018] In an embodiment, the photocatalyst further includes an auxiliary catalyst that includes
at least one of a noble metal and nickel.
[0019] In an embodiment, the photocatalyst further includes an inorganic carrier material
that is fixed to a base body with an inorganic adhesive.
[0020] For example, a photocatalytic ignition system may be provided that basically comprises
an ignition chamber, a photocatalyst and a light source. The ignition chamber is configured
to receive an air fuel mixture. The photocatalyst is arranged in the ignition chamber
to contact an air fuel mixture. The light source is arranged to shine light on the
photocatalyst. The photocatalyst includes a photocatalytic material having an oxygen
absorbing and a desorbing function. The photocatalytic ignition system is capable
of igniting a lean air fuel mixture with a greatly reduced amount of light energy.
[0021] Within the scope of this application it is envisaged that the various aspects, embodiments,
examples, features and alternatives set out in the preceding paragraphs, in the claims
and/or in the following description and drawings may be taken individually or in any
combination thereof.
[0022] The present invention will now be described, by way of example only, with reference
to the accompanying drawings in which:
Figure 1 is a system diagram showing a photocatalytic ignition system in accordance
with one embodiment; and
Figure 2 is a graph showing a pressure change inside the ignition chamber in Working
Example 1.
[0023] Selected embodiments of the present invention will now be explained with reference
to the drawings. It will be apparent to those skilled in the art from this disclosure
that the following descriptions of the embodiments of the present invention are provided
for illustration only and not for the purpose of limiting the invention as defined
by the appended claims and their equivalents.
[0024] Referring initially to Figure 1, a photocatalytic ignition system is illustrated
in accordance with a first embodiment. This photocatalytic ignition system is a system
that ignites a mixture of fuel gas and air using a photocatalyst and a light source.
In this photocatalytic ignition system, the light source serves the function of supplying
light to the photocatalyst and the photocatalyst contains a photocatalytic material
that has both a photocatalytic function and an oxygen absorbing desorbing function.
With this photocatalytic ignition system, an air fuel mixture can be headed in a localized
fashion and ignited. As a result, a photocatalytic ignition system can be provided
which can ignite a lean air fuel mixture with a much smaller amount of light energy
than previously proposed systems. In both the claims and the description, concentrations,
content amounts, and filling amounts expressed as a value followed by "%" are mass
percentages unless otherwise specified.
[0025] In this embodiment, there are no particular limitations on the fuel contained in
the air fuel mixture. Normally, the fuel used is a hydrocarbon or alcohol based fuel.
In particular, examples of fuels used in internal combustion engines include gasoline,
diesel fuel, heavy oil, biogasoline, liquefied petroleum gas (LPG), liquefied natural
gas (LNG), methanol, and ethanol.
[0026] Any light source is acceptable so long as it can supply a light to the photocatalyst
that activates the photocatalytic material used. A light source that emits ultraviolet
light, visible light, infrared light, or a combination of these is acceptable. There
are previously known light sources available that can be used as the light source.
Typically, if the light has a wavelength corresponding to an energy level equal to
or higher than the band gap energy of the photocatalytic material, then electrons
in the valence band of the photocatalytic material will be excited into the conduction
band and holes will develop in the valence band, thus promoting a photocatalytic reaction.
[0027] While the photocatalytic material is a primary component of the photocatalyst that
is used to ignite the fuel and air mixture, it is also acceptable to include other
component such as a photothermal conversion material, an auxiliary catalyst, or an
inorganic carrier material as needed and/or desired. The photocatalytic material contained
in the photocatalyst will now be explained. There are no particular limits on the
photocatalytic material so long as it causes a photocatalytic reaction to occur when
light is shone thereon and it has an oxygen absorbing desorbing function. To ignite
the fuel and air mixture, the photocatalytic material advantageously has an oxygen
absorbing and a desorbing function, which will now be explained using a hypothetical
example.
[0028] When light is shown onto the photocatalyst, electrons (e-) and holes are produced
on the surface of the photocatalyst. The electrons produced react with oxygen molecules
(O
2) in the air to make O
2-. The O
2- receives another electron and forms O
-, and the O
- pulls a hydrogen atom from the hydrocarbon of the fuel and causes the hydrocarbon
of the fuel to become a hydrocarbon radical, thus promoting combustion via a chain
reaction.
[0029] Meanwhile, since photocatalytic material has the oxygen absorbing desorbing function,
the photocatalytic material desorbs oxygen in the O
2- state. In such a case, there is the possibility that the O
2- will react with holes at the surface of the photocatalyst and lose an electron, causing
an O
- to be produced. The O
- is an active species necessary for the chain reaction described above. Thus, it is
believed that the oxygen absorbing desorbing function causes more O
- to be produced than would occur otherwise, thus accelerating combustion. As a result,
a lean air fuel mixture can be ignited with a greatly reduced amount of light energy.
[0030] Specific examples of photocatalytic materials having both an oxygen absorbing and
a desorbing function include cerium oxide (CeO
2), titanium oxide (TiO
2), copper oxide (CuO), and any combination of these materials. For example, cerium
oxide can be made to absorb and desorb oxygen in accordance with an oxidation/reduction
atmosphere by utilizing an oxidation/reduction cycle between the quadrivalent and
trivalent states of cerium. When cerium oxide is used as a photocatalytic material
having an oxygen absorbing and a desorbing function, it is beneficial for the average
particle size of the cerium oxide to be 20 nm or smaller. It is sometimes difficult
to obtain sufficient performance when the average particle size is larger than 20
nm. By making the particle size smaller, the movement distances of electrons and holes
are shorter during a photocatalytic reaction and it is less likely that deactivation
will occur. This phenomenon is not limited to cerium oxide. Additionally, when nanoparticles
of cerium oxide crystallize having high crystallinity and few defects are used, electrons
and holes are less likely to become deactivated in the process of moving along the
surface of the photocatalyst. For these reasons, cerium oxide having the aforementioned
particle size is an excellent material to use as the photocatalytic material.
[0031] The photothermal conversion material will now be explained. The photothermal conversion
material is advantageously used as part of the photocatalyst along with the photocatalytic
material. There are no particular limitations on the photothermal conversion material
so long as it is a material that functions to convert light into heat and emit the
heat. For example, transition metal compounds that can be used as a photothermal conversion
material include oxides of transition metals other than cerium, titanium, and copper,
sulfides of transition metals (including cerium, titanium, and copper), and nitrides
of transition metals (including cerium, titanium, and copper). Any combination of
these oxides, sulfides, and nitrides is also acceptable.
[0032] In this photocatalytic ignition system, particularly favorable results can be obtained
by using iron (Fe) and/or vanadium (V) as a transition metal in the aforementioned
transition metal compound of the photothermal conversion material. Compounds (i.e.,
oxide, sulfide, and nitride compounds) of iron and vanadium emit heat when they absorb
light. The reason for the heat emission is thought to be either (1) that excitation
energy is converted to thermal energy or (2) that the compound undergoes a reduction
reaction when it absorbs light and then emits heat when it oxidizes again due to oxygen
in the vicinity. Either way, the compound emits heat and heats the photocatalytic
material, thereby causing the temperature of the catalyst surface to rise. It is believed
that, as a result, the reaction is accelerated and the oxidizing performance, i.e.,
the igniting performance, is improved.
[0033] Among compounds of iron and vanadium, an oxide of iron is particularly good. Particularly
good results are obtained when an iron oxide photothermal conversion material is used
together with cerium oxide as the photocatalytic material. In such a case, it is acceptable
for the iron (Fe) and the cerium (Ce) to form a composite oxide. In this invention,
it is advantageous for the content ratio of cerium and iron (Ce/Fe) to be a mole ratio
in the range of 2/8 to 8/2. If the mole ratio departs from this range such that the
amount of iron is too small, then the heating effect will not be obtained and the
performance will not be sufficiently improved. Conversely, if the amount of iron is
too large, then the ignition performance may decline.
[0034] The auxiliary catalyst will now be explained. The auxiliary catalyst is used as part
of the photocatalyst along with the photocatalytic material. During the photocatalytic
reaction, it functions to collect separated charges such that recombination of electrons
and holes is suppressed, thereby promoting charge separation. More specifically, separated
charges resulting from light absorption move to the surface of the catalyst and activate
the reactants. If recombination occurs during the movement, then deactivation will
occur. Any material that can separate charges effectively and suppress recombination,
thereby collecting charges (electrons), can be used as an auxiliary catalyst.
[0035] There are no particular limitations on the material used as the auxiliary catalyst.
Examples include at least one of or any combination of the noble metals and nickel,
more specifically at least one of or any combination of rhodium (Rh), cobalt (Co),
copper (Cu), ruthenium (Ru), palladium (Pd), iridium (Ir), platinum (Pt), and nickel
(Ni).
[0036] The inorganic carrier material will now be explained. The inorganic carrier material
is used as part of the photocatalyst along with the photocatalytic material. The inorganic
carrier material functions to support and secure the photocatalytic material. Specific
examples include alumina (Al
2O
3), zirconia (ZrO
2), and magnesia (MgO
2).
[0037] In this photocatalytic ignition system, a base body, typically a substrate plate,
can be used to secure the photocatalyst. In such a case, it its beneficial to secure
the photocatalyst to the base body with an inorganic adhesive. The inorganic adhesive
should be configured to adhere to both the photo catalyst (i.e., the photocatalytic
material and the inorganic carrier material) and the base body in order to prevent
the photocatalyst from peeling or cracking. Examples of inorganic adhesives include
alumina (Al
2O
3) and zirconia (ZrO
2).
[0038] Figure 1 is a system diagram showing an embodiment of a photocatalytic ignition system.
As shown in Figure 1, this photocatalytic ignition system comprises a photocatalyst
10 and a laser device 20 constituting a light source.
[0039] The photocatalyst 10 is on a substrate plate 11 that is housed inside an ignition
chamber 30. The ignition chamber 30 is configured such that a mixture of fuel and
air can be supplied thereto as indicated with an arrow F and exhaust gas can be discharged
therefrom as indicated with an arrow E. Internal pressure of the ignition chamber
30 can be detected with a pressure sensor 32, and laser light from the laser device
20 can be shone into the ignition chamber 30 through a light inlet window 31 made
of quartz glass.
[0040] The laser light emitted from the laser device 20 is reflected by a reflection mirror
21 and the intensity of the laser light is adjusted by an attenuator 22. The laser
light passes through a light collecting lens 23 (f = 200), and is directed through
the light inlet window 31 into the ignition chamber 30, where the light strikes the
photocatalyst 10.
[0041] As explained above, when the laser light shines on the photocatalyst 10, the photocatalyst
10 is activated and causes localized heating of the air fuel mixture, thereby igniting
the air fuel mixture.
[0042] Working examples of one photocatalytic ignition system and comparative examples will
now be explained in detail. The photocatalytic ignition system is not limited by these
working examples.
Working Example 1
[0043] The photocatalytic ignition system shown in Figure 1 was fabricated and the performance
thereof was evaluated. The procedures of the fabrication and performance evaluation
of the system will now be explained.
[0044] An aluminum plate having a diameter of 60 mm was used as the substrate plate 11.
Oil was removed from the aluminum plate by treating it with alcohol and, afterwards,
an inorganic adhesive (main ingredient: α alumina) was coated onto the aluminum plate.
Next, the photocatalyst 10 was made by spraying cerium oxide sol having a particle
size of 20 nm to a thickness of several micrometers and firing to remove moisture.
[0045] The laser light was provided by a Nd-YAG laser (355 nm) and pulsed at a pulse width
of 5 to 7 nsec. The laser light was passed through a 355 nm wavelength separator mirror,
an attenuator (1/2 wavelength plate and polarizer plate), a light collecting lens
(f = 200), and a quartz glass window and shone onto the photocatalyst inside the ignition
chamber. A mixture of CH
4 and air was supplied to the inside of the ignition chamber and controlled with a
mass flow controller to a ratio of 10 % by volume of CH
4 to air. The pressure inside the chamber was 0.2 MPa and the temperature was room
temperature. The volume of the ignition chamber was approximately 600 cc.
[0046] After the inside of the ignition chamber was evacuated with a vacuum pump, the mixture
of CH
4 and air was supplied and the laser was energized. The laser light was shone while
changing the energy of the laser in the following sequence: 38.6 mJ → 35.7 mJ → 31.9
mJ → 25.1 mJ. The irradiation energy of the laser light was measured with a power
meter. The occurrence of ignition (combustion) was confirmed based on the internal
pressure of the ignition chamber. The pressure change during combustion was measured
by sampling a voltage from the pressure sensor at five (5) msec intervals. Figure
2 shows the pressure change measurement results that were obtained. Table 1 shows
the minimum ignition energy (mJ) for the photocatalyst used in this working example.
Working Example 2
[0047] An aqueous solution was prepared with ferric nitrate and cerium nitrate at a mole
ratio of Fe to Ce (Fe/Ce) equal to 0.8/0.2. The solution was agitated one day and
one night while gradually dripping in an aqueous solution containing 28% ammonia such
that a pH of 8 was achieved. The resulting solid material was then filtered out, rinsed
with deionized water, and heated to 600 °C for five hours to obtain Fe
0.8Ce
0.2. The Fe-Ce material was used as the photocatalyst. Otherwise, the same operations
as were performed in Working Example 1 were repeated. Table 1 shows the minimum ignition
energy (mJ) for the photocatalyst used in this working example.
Working Example 3
[0048] An aqueous solution was prepared with ferric nitrate and cerium nitrate at a mole
ratio of Fe to Ce (Fe/Ce) equal to 0.2/0.8. Otherwise the same operations as were
performed in Working Example 2 were repeated. The minimum ignition energy (mJ) is
shown in Table 1.
Working Example 4
[0049] Titanium oxide having a particle size of several micrometers was used as the photocatalyst.
Otherwise, the same operations as were performed in Working Example 1 were repeated.
The minimum ignition energy (mJ) is shown in Table 1.
Comparative Example 1
[0050] A photocatalyst was not fabricated (an aluminum substrate plate was not installed).
Otherwise, the same operations as in Working Example 1 were repeated. The minimum
ignition energy (mJ) is shown in Table 1.
Comparative Example 2
[0051] An aluminum substrate plate was installed but a photocatalyst was not fabricated.
Otherwise, the same operations as in Working Example 1 were repeated The minimum ignition
energy (mJ) is shown in Table 1.
Comparative Example 3
[0052] An iron oxide was used as a photocatalyst. Otherwise, the same operations as in Working
Example 1 were repeated. The minimum ignition energy (mJ) is shown in Table 1.
Table 1
Working Example 1 |
31.9 |
Working Example 2 |
25.1 |
Working Example 3 |
28.2 |
Working Example 4 |
33.0 |
Comparative Example 1 |
38.6 |
Comparative Example 2 |
36.0 |
Comparative Example 3 |
35.3 |
[0053] The photocatalyst used in Comparative Example 1 was iron oxide and the photocatalyst
used in Working Example 1 was cerium oxide (photocatalytic material). A comparison
of Comparative Example 1 and Working Example 1 indicates that the amount of energy
required to ignite the air fuel mixture can be reduced by using a material having
an oxygen absorbing desorbing function as the photocatalytic material.
[0054] The photocatalysts used in Working Examples 2 and 3 were made of cerium oxide (photocatalytic
material) and iron (photothermal conversion material). A comparison of Working Example
1 to Working Examples 2 and 3 indicates that the amount of energy required to ignite
the air fuel mixture can be reduced even further by using a material having a photothermal
conversion function as the photocatalytic material. The photocatalyst used in Working
Example 4 was made of titanium oxide (photocatalytic material) only. A comparison
of Working Example 1 and Working Example 4 indicates that the air fuel mixture can
be ignited with a smaller amount of energy by using cerium oxide as the photocatalytic
material.
[0055] In understanding the scope of the present invention, the term "comprising" and its
derivatives, as used herein, are intended to be open ended terms that specify the
presence of the stated features, elements, components, groups, integers, and/or steps,
but do not exclude the presence of other unstated features, elements, components,
groups, integers and/or steps. The foregoing also applies to words having similar
meanings such as the terms, "including", "having" and their derivatives.
[0056] While only selected embodiments have been chosen to illustrate the present invention,
it will be apparent to those skilled in the art from this disclosure that various
changes and modifications can be made herein without departing from the scope of the
invention as defined in the appended claims. For example, the size, shape, location
or orientation of the various components can be changed as needed and/or desired.
Components that are shown directly connected or contacting each other can have intermediate
structures disposed between them. The functions of one element can be performed by
two, and vice versa. The structures and functions of one embodiment can be adopted
in another embodiment. It is not necessary for all advantages to be present in a particular
embodiment at the same time. Every feature which is unique from the prior art, alone
or in combination with other features, also should be considered a separate description
of further inventions by the applicant, including the structural and/or functional
concepts embodied by such feature(s). Thus, the foregoing descriptions of the embodiments
according to the present invention are provided for illustration only, and not for
the purpose of limiting the invention as defined by the appended claims and their
equivalents.
1. An apparatus comprising:
an ignition chamber for receiving an air fuel mixture;
a photocatalyst arranged in the ignition chamber for contacting the air fuel mixture;
and
a light source for shining light on the photocatalyst,
wherein the photocatalyst comprises a photocatalytic material having an oxygen absorbing
and a desorbing function.
2. An apparatus as claimed in claim 1, wherein the photocatalytic material is at least
one selected from a group consisting of cerium oxide, titanium oxide and copper oxide.
3. An apparatus as claimed in claim 1 or claim 2, wherein the photocatalytic material
comprises cerium oxide with an average particle size of 20 nm or smaller.
4. An apparatus as claimed in any preceding claim, wherein the photocatalyst comprises
a photothermal conversion material that includes at least one transition metal compound
selected from a group consisting of transition metal sulfides, transition metal nitrides
and oxides of transition metals other than cerium, titanium and copper.
5. An apparatus as claimed in claim 4, wherein the photothermal conversion material comprises
at least one of iron and vanadium as a transition metal of the transition metal compound.
6. An apparatus as claimed in claim 4 or claim 5, wherein the photocatalytic material
comprises cerium oxide, the photothermal conversion material is an oxide of iron,
and the mole ratio of cerium to iron contained in the photocatalyst lies in the range
of 2/8 to 8/2.
7. An apparatus as claimed in any preceding claim, wherein the photocatalyst comprises
an auxiliary catalyst that includes at least one of a noble metal and nickel.
8. An apparatus as claimed in any preceding claim, wherein the photocatalyst comprises
an inorganic carrier material that is fixed to a base body with an inorganic adhesive.
9. A photocatalytic ignition system comprising an apparatus as claimed in any preceding
claim.
10. An engine comprising an apparatus or a system as claimed in any preceding claim.
11. A vehicle having an apparatus, a system or an engine as claimed in any preceding claim.