This application claims priority from UK patent application no. 1010741.5 filed on 25 June 2010, UK patent application no. 1010742.3 filed on 25 June 2010, UK patent application no. 1010745.6 filed on 25 June 2010, UK patent application no. 1010743.1 filed on 25 June 2010 and UK patent application no. 1101642.5 filed on 31 January 2011. The contents of each aforementioned priority-forming application are incorporated herein in their entirety by reference.

Summary of the Invention

This invention relates to organic light emitting compositions, devices containing the same, and methods of making said devices.

Background of the Invention

Electronic devices comprising active organic materials are attracting increasing attention for use in devices such as organic light emitting diodes, organic photovoltaic devices, organic photosensors, organic transistors and memory array devices. Devices comprising organic materials offer benefits such as low weight, low power consumption and flexibility.

Moreover, use of soluble organic materials allows use of solution processing in device manufacture, for example inkjet printing or spin-coating.

A typical organic light-emissive device ("OLED") is fabricated on a glass or plastic substrate coated with a transparent anode such as indium-tin-oxide ("ITO"). A layer of a thin film of at least one electroluminescent organic material is provided over the first electrode. Finally, a cathode is provided over the layer of electroluminescent organic material. Charge transporting, charge injecting or charge blocking layers may be provided between the anode and the electroluminescent layer and / or between the cathode and the electroluminescent layer.

In operation, holes are injected into the device through the anode and electrons are injected into the device through the cathode. The holes and electrons combine in the organic electroluminescent layer to form an excitons which then undergo radiative decay to give light. In WO90/13148 the organic light- emissive material is a conjugated polymer such as poly(phenylenevinylene). In US 4,539,507 the organic light-emissive material is of the class known as small molecule materials, such as tris-(8-hydroxyquinoline) aluminium ( "Alq ₃ " ). These materials electroluminesce by radiative decay of singlet excitons (fluorescence) however spin statistics dictate that up to 75% of excitons are triplet excitons which undergo non-radiative decay, i. e. quantum efficiency may be as low as 25% for fluorescent OLEDs- see, for example, Chem. Phys. Lett., 1993,210, 61, Nature (London), 2001,409, 494, Synth. Met., 2002,125, 55 and references therein.

It has been postulated that the presence of triplet excitons, which may have relatively long- lived triplet excited states, can be detrimental to OLED lifetime as a result of triplet-triplet or triplet-singlet interactions ("lifetime" as used herein in the context of OLED lifetime means the length of time taken for the luminance of the OLED at constant current to fall by 50% from an initial luminance value, and "lifetime" as used herein in the context of lifetime of a triplet excited state means the half-life of a triplet exciton). US 2007/145886 discloses an OLED comprising a triplet-quenching material to prevent or reduce triplet-triplet or triplet- singlet interactions between molecules in the excited state by quenching undesirable triplet excited states without quenching the excited singlet states that decay by fluorescent emission.

WO 2005/043640 discloses that blending a perylene derivative with an organic light-emissive material in an organic light-emissive device can give a small increase in the lifetime of the device. However, while higher concentrations of perylene derivative give greater improvements in lifetime this results in a significant red-shift in the emission spectrum.

US 2007/145886 discloses an OLED comprising a triplet-quenching material to prevent or reduce triplet-triplet or triplet-singlet interactions.

US 2005/095456 discloses an OLED having a light-emitting layer comprising a host material, a dye or pigment and an additive exhibiting an absorption edge of which energy level is higher than that of an absorption edge of the dye or the pigment

However, quenching of triplet excitons as described in US 200/145886 inevitably means that the energy of the triplet excitons is lost in non-light emitting pathways (such as heat).

Summary of the Invention The present inventors have identified a number of pathways by which triplet excitons may be caused to undergo decay in order to reduce or eliminate decay by pathways that cause a drop in device lifetime. Significantly, some of these pathways allow for radiative exciton decay that can provide for better device efficiency as compared to non-radiative decay pathways.

In a first aspect, the invention provides a composition for use in an organic light-emitting device comprising a fluorescent light-emitting material and a triplet-accepting material wherein:

2 x T _1A ≥ S _1A > SiE, or TiA + T _1E > S _1A > S _1E

in which:

TiA represents a triplet excited state energy level of the triplet-accepting material;

TIE represents a triplet excited state energy level of the light-emitting material;

represents a singlet excited state energy level of the triplet-accepting material; and

SiE represents a singlet excited state energy level of the light-emitting material;

and wherein light emitted by the composition upon excitation includes delayed fluorescence.

Optionally, at least 10 %, optionally at least 20 %, of the luminescent intensity of light emitted by the composition upon excitation is delayed fluorescence.

Optionally, a continuous excitation of the composition for a period sufficient to cause the luminescent intensity of the composition to fall by 50 % from an initial luminescent intensity results in emission of delayed fluorescence for the entire period following intial emission of delayed fluorescence following initial excitation of the composition.

Optionally:

in which: knE-TiA represents the rate constant for transfer of a triplet exciton on the light-emitting material to the triplet- accepting material;

k-riE-soE represents the rate constant for decay of a triplet exciton on the light-emitting material to the ground state of the light emitting material. Optionally:

klTA > kr A-SOA

in which krrA represents the rate constant for triplet-triplet annihilation between two triplet excitons on two triplet-accepting materials, or between a triplet exciton on the triplet accepting material and a triplet exciton on the light-emitting material; and kn _A -so _A represents the rate constant for decay of a triplet exciton on the triplet-accepting material to the ground state of the triplet-accepting material.

Optionally, at least some of the triplet-accepting material comprises formula (II):

TAU-Sp-TAU

(Π)

wherein TAU represents the triplet-accepting material, and Sp represents a spacer group. Optionally, Sp comprises an arylene group.

Optionally, the at least some of the triplet-accepting material comprises formula (Ila):

TQ-Ar-TQ

(Ila)

wherein Ar represents an optionally substituted arylene group.

Optionally, Ar is selected from the group consisting of: phenyl, biphenyl, terphenyl and fluorene.

Optionally, the triplet-accepting material is mixed with the light emitting material and any other component or components of the composition.

Optionally, the triplet-accepting material is bound to light emitting material or, if present, to another component of the composition.

Optionally, the composition comprises at least one of a hole transporting material and an electron transporting material and wherein the triplet-accepting unit is bound to at least one of the hole transporting material, the electron transporting material and the light-emitting material.

Optionally, the triplet-accepting unit is bound to the light emitting material.

Optionally, the light emitting material is a light-emitting polymer and the triplet-accepting material is a repeat unit in the main chain of the light-emitting polymer or a side-group or end-group of the light-emitting polymer.

Optionally, the light-emitting polymer comprises a light-emitting repeat unit and at least one of repeat units providing electron transport and repeat units providing hole transport, wherein the triplet-accepting material is bound to at least one of the light-emitting repeat unit, the repeat unit providing electron transport and the repeat unit providing hole transport.

Optionally, the triplet-accepting material is substituted with one or more solubilising groups.

Optionally, the solubilising group is selected from alkyl and alkoxy.

Optionally, the light-emitting material is a light-emitting polymer comprising arylamine repeat units.

Optionally, the arylamine repeat units are units of formula (V):

(V)

wherein Ar ¹ and Ar ² are optionally substituted aryl or heteroaryl groups, n is greater than or equal to 1, preferably 1 or 2, and R is H or a substituent.

Optionally, the polymer comprises aryl or heteroaryl repeat units, optionally repeat units of formula (IV):

(IV) wherein R ¹ and R ² are independently H or a substituent, and R ¹ and R ² may be linked to form a ring.

Optionally, the triplet-accepting material is present in an amount of at least 0.1 mol %.

Optionally, the composition has a photoluminescent light emission peak wavelength in the range of 400 to 500 nm.

Optionally, the triplet-accepting material does not comprise a perylene.

In a second aspect the invention provides a solution comprising a solvent and a composition according to the first aspect.

In a third aspect the invention provides an organic light-emitting device comprising an anode, a cathode and a light-emitting layer between the anode and cathode, wherein the light- emitting layer comprises a composition according to the first aspect.

In a fourth aspect the invention provides a method of forming an organic light-emitting device according to the third aspect comprising the steps of depositing the solution according to the second aspect and evaporating the solvent.

In a fifth aspect the invention provides use of a triplet-accepting material for mediating delayed fluorescence by triplet-triplet annihilation of triplet excitons generated by a fluorescent light-emitting material in a composition comprising the triplet-accepting material and the fluorescent light-emitting material.

The composition of the fifth aspect may optionally include any feature described with respect to the first aspect. For example, the triplet-accepting material may be physically mixed with the fluorescent light-emitting material or may be chemically bound to the fluorescent light- emitting material. Optionally, the fluorescent light-emitting material is a polymer and the triplet-accepting material is provided as a repeat unit in the polymer main chain, a side group pendent from the polymer main chain or a polymer end-group.

Brief Description of the Drawings

Figure 1 is a schematic illustration of prior art triplet quenching;

Figure 2 is a schematic illustration of a first triplet-triplet annihilation mechanism according to an embodiment of the invention; Figure 3 illustrates a second triplet-triplet annihilation according to an embodiment of the invention; and

Figure 4 illustrates an organic light-emitting device according to an embodiment of the invention.

Figure 5 illustrates external quantum efficiency of a device according to an embodiment of the present invention.

Figure 6 illustrates the quasi-cw current induced excited state absorption curves of a device according to an embodiment of the present invention.

Figure 7 illustrates time resolved electroluminescence during the turn off of a device according to an embodiment of the present invention.

Figure 8 illustrates decay of device luminance with time and change in efficiency with time of a device according to an embodiment of the present invention.

Figure 9 illustrates delayed emission of a device according to an embodiment of the present invention.

Figure 10 illustrates delayed fluorescence obtained from an embodiment of the present invention.

Detailed Description of the Invention

Figure 1 illustrates a mechanism of energy transfer according to a prior art arrangement. For the avoidance of any doubt energy level diagrams herein, including Figure 1, are not drawn to any scale. Figure 1 illustrates energy transfer for an OLED provided with a light emitting material having a singlet excited state energy level SIE and a singlet ground state energy level SOE- Singlet excitons having energy S _1E decay by emission of fluorescent light hv, illustrated by the solid arrow between Si _E and SOE in Figure 1. Triplet-triplet exciton interactions or triplet-singlet exciton interactions may create "super-excited" states on the light-emitting material. Without wishing to be bound by any theory, it is believed that formation of these highly energetic "super-excited" states on the light emitting material may be detrimental to operational lifetime of the material. Moreover, the triplet-triplet interactions may form singlet excitons that undergo radiative decay which adds to the luminescence of the OLED but which tends to occur only at the start of OLED driving and tails off very rapidly to give a steep drop in initial luminance of the OLED. However, by providing a triplet quenching material having an excited triplet state energy level that is lower than T _1E , it is possible for triplet excitons to be transferred for non-radiative quenching to the triplet quencher, the alternative of radiative decay from T _1E to S ₀ E, illustrated by a dotted line in Figure 1, being a spin-forbidden process.

The triplet quenching material in this illustration is selected so as to have a singlet excited state energy level SiQ that is higher than the singlet excited state energy level SIE in order to substantially or completely prevent transfer of singlet excitons from S _I E to SIQ. Although it may be preferable for energy level S _I Q to be greater than S _I E, it will be appreciated that this is not essential in order for triplet quenching to occur. Preferably, SIQ is at least kT higher in energy than in order to prevent any substantial back-transfer of excitons. Likewise, TIE is preferably at least kT higher in energy than TiQ.

Quenching in this way inevitably means that the energy of the triplet exciton formed at T^ is lost to radiative decay pathways.

Figure 2 illustrates a first energy transfer mechanism for an OLED according to an

embodiment of the invention _. in which the OLED comprises a light-emitting material and a triplet-accepting material. The light emitting material and triplet-accepting material may be separate units in the form of a blend of light-emitting molecules and triplet-accepting molecules. Alternatively, the triplet-accepting material may be bound to the light-emitting material; for example, the light-emitting material may comprise a conjugated or non- conjugated polymer comprising light-emitting repeat units and triplet-accepting repeat units.

According to this embodiment, triplet-triplet annihilation (TTA), caused by an interaction between two triplet-accepting units, results in a triplet-triplet annihilated singlet exciton having an energy of up to 2 x T _1A , wherein T _1A represents the triplet excited state energy level of the triplet-accepting material. This singlet exciton, formed on a first of the two triplet- accepting units, has energy level S„A that is higher in energy than S _1A and SIE and so it may transfer to S _I A and then to S^ from which light hv may be emitted as delayed fluorescence. The triplet exciton on the second of the two triplet-accepting units may decay to the ground state TOA-

Initially, the triplet exciton formed at T _I E is transferred to T _1A . By providing a triplet- accepting material having energy level TIA that is lower than Τ^, rapid transfer of excitons from T E to T _1A may occur. This transfer is relatively rapid compared to the rate of decay of triplet excitons from T _I E to SOE, illustrated by a dotted arrow in Figure 1, which is a spin- forbidden process. The energy gap between T _I E and T _1A is preferably greater than kT in order to avoid back-transfer of excitons from Ti _A to TIE- Likewise, the energy gap between S _1A and is preferably greater than kT in order to avoid back-transfer of excitons from S _\ E to S _{X A} .

A pathway for decay of the triplet exciton on T _1A in competition with triplet-triplet annihilation is the non-radiative (quenching) pathway to S ₀ A described above with respect to Figure 1. A number of measures may be taken to maximise the probability of TTA rather than decay to SOA, in particular: i) The triplet-absorbing material may be selected such that triplet excitons on T _1A have a relatively long lifetime TT _A - A relatively long lifetime not only means that the rate of decay to SOA is relatively slow but also that the likelihood of TTA is relatively high.

ii) The concentration of triplet-absorbing material in the light-emitting layer may be relatively high, for example greater than 1 mol %, for example in the range of 0.1-10% or 1-10 mol . iii) Two or more triplet-accepting materials may be provided in close proximity, for example as described below with reference to units of formula (II).

Each of these measures may be used alone or in combination.

Figure 3 illustrates a second energy transfer mechanism for a further embodiment of the invention. As set out above with respect to Figure 2, The light emitting material and triplet- accepting material may be separate units in the form of a blend of light-emitting molecules and triplet accepting molecules. Alternatively, the triplet-accepting material may be bound to the light-emitting material; for example, the light-emitting material may comprise a conjugated or non-conjugated polymer comprising light-emitting repeat units and triplet- accepting repeat units. In one embodiment, the light-emitting material is an at least partially conjugated polymer, i.e. at least some repeat units in the polymer backbone are conjugated to adjacent repeat units.

In this case, triplet-triplet annihilation occurs between the triplet exciton of energy Ti _A located on the triplet accepting material and the triplet exciton of energy located on the light-emitting material. It will be appreciated that this results in a triplet-triplet annihilated singlet exciton having an energy of up to Tm + ^. This singlet exciton is higher in energy than SiE and so it may transfer its energy to SiE from which light hv may be emitted as delayed fluorescence.

In Figures 2 and 3, although it may be preferable for energy level SIA to be greater than SIE, it will be appreciated that this is not essential in order for triplet absorption to occur.

Without wishing to be bound by any theory, it is believed that avoiding formation of super- excited states on the light-emitting material formed during OLED driving may improve device lifetime. Moreover, by utilising a triplet accepting material to generate TTA and produce stable, delayed fluorescence it is possible to improve efficiency as compared to a device in which triplet excitons are quenched (as illustrated in Figure 1) or as compared to a device in which there is no triplet accepting unit wherein intensity of delayed fluorescence may drop sharply following initial OLED driving.

In Figures 2 and 3, TTA has been described with respect to absorber unit-absorber unit triplet annihilation and absorber unit-emitter unit triplet annihilation mechanisms respectively, however it will be appreciated that it is possible for both mechanisms to operate in the same device, and that the amount of delayed fluorescence from each of these two mechanisms will depend on factors such as the concentration of light emitting units, the concentration of triplet accepting units, and the excited state lifetime of triplet excitons on the light emitting unit and the triplet accepting unit. Measures described above with reference to Figure 2 may be employed to increase the probability of TTA.

The rate constant of transfer of triplet excitons from the light-emitting material to the triplet- accepting material may be selected so as to be greater than the rate constant of quenching of triplet excitons. Light emitted from light-emitting compositions of the invention may include delayed fluorescence as described above, as well as fluorescence arising directly from recombination of holes and electrons on the light-emitting material ("prompt fluorescence").

The skilled person will be aware of methods to determine the presence of delayed

fluorescence in light emitted from a light-emitting composition, for example by measuring light emission from a light-emitting composition following prompt fluorescence.

Time resolved electroluminescent spectra may be taken during the turn off of the prototypical device; after turn off of the current an initial rapid decay of the luminance on a similar timescale to the RC time constant of the device followed by a residual signal in the EL which decays in a few microseconds. Generally slow transient emissions in OLEDs are ascribed to either the recombination of charges from deep traps or interfacial charge layers or TTA (see Kondakov, D.Y. Characterization of triplet-triplet annihilation in organic light-emitting diodes based on anthracene derivatives. J. Appl. Phys. 102, 114504-5 (2007), Sinha, S., Rothe, C, Guentner, R., Scherf, U. & Monkman, A.P. Electrophosphorescence and Delayed Electroluminescence from Pristine Polyfluorene Thin Film Devices at Low Temperature. Physical Review Letters 90, 127402 (2003), and Sinha, S., Monkman, A.P., Guntner, R. & Scherf, U. Space-charge-mediated delayed electroluminescence from polyfluorene thin films. Appl. Phys. Lett. 82, 4693-4695 (2003)).

In order to distinguish between the two mechanisms the same transient electroluminescence trace may been measured with the application of a 10V reverse bias pulse 100ns after the turn off of the device current, this pulse will remove, or at least perturb significantly, any trapped charge contribution to the decay of the luminance. If the decay of EL after the reverse bias pulse is unchanged compared to the standard decay shape then it may be concluded that the recombination of trapped charge is not a significant contributor to the residual luminance signal but is rather due to delayed fluorescence (Popovic, Z.D. & Aziz, H. Delayed electroluminescence in small-molecule-based organic light-emitting diodes: Evidence for triplet-triplet annihilation and recombination-center-mediated light-generation mechanism. J. Appl. Phys. 98, 013510-5 (2005)). Triplet-accepting unit

The triplet-accepting unit as used may be a compound that is chemically unbound to, but physically mixed with, the light-emitting material and any other components of the light- emitting composition, such as one or more charge-transporting materials (e.g. one or both of hole transporting and electron transporting materials). Alternatively, the triplet-accepting unit may be bound , in particular covalently bound, to the light-emitting material or another component of the composition directly or through a spacer group.

In the case where the triplet-accepting unit is blended with the light-emitting material, the unit is preferably substituted with solubilising groups. Exemplary triplet- accepting compounds include aromatic or heteroaromatic compounds comprising one or more mono- or polycyclic rings, and optionally including one or more alkenyl or alkynyl groups, for example polyaromatic hydrocarbons such as anthracenes and anthanthrenes and derivatives thereof; distyryl aryls and derivatives thereof such as distyrylbenzenes, distyrylbiphenyls, stilbenes, fulvenes, dibenzofulvenes, linear polyenes (from 2 to 6 alkenes) including cyclic polyenes such as cyclooctatetraene.

Any of these compounds may optionally be substituted, for example substituted with one or more solubilising groups such as alkyt, and may be provided as a component of a larger structure, for example as a repeat unit of a polymer.

Further materials having appropriate singlet and triplet photophysical properties are described in Handbook of Photochemistry, 2 ^nd Edition, Steven L Murov, Ian Carmichael and Gordon L Hug, the contents of which are incorporated herein by reference, each of which compound may optionally be substituted, for example substituted with alkyl groups. In one

embodiment, the triplet-accepting unit does not comprise a polycyclic aromatic hydrocarbon unit comprising more than 12 sp ² hybridised carbon atoms.

Exemplary anthanthrene compounds include the following:

wherein Ak is alkyl, in particular branched or straight chain C^o alkyl. Particularly preferred alkyl groups are n-butyl, t-butyl, n-hexyl and n-octyl.

In the case where the light-emitting material is a polymer, the triplet-accepting unit may be a compound that is physically mixed with the light emitting polymer, or it may be provided as repeat units in the polymer main chain, one or more side groups pendant from the polymer main chain, or polymer end-groups.

The triplet-accepting unit may be bound into the main chain of a light-emitting polymer by polymerising a monomer comprising the triplet accepting repeat unit substituted with at least two polymerisable groups, such as leaving groups capable of participating in a metal- catalysed cross-coupling reaction (it will be appreciated that polymerisation of a monomer comprising more than two leaving groups will create a branch point in the polymer if more than two of the leaving groups react). Substitution of leaving groups on sp ² carbon atoms of the triplet-accepting unit may be used for this purpose. Exemplary leaving groups include halogen and boronic acid or ester groups for use in Suzuki or Yamamoto polymerisation reactions, described in more detail below. The triplet-accepting unit may be bound to any repeat unit of the light-emitting polymer described below, for example to a light-emitting repeat unit, an electron-transporting repeat unit and / or a hole transporting repeat unit. In one embodiment, this polymer comprises a triplet-accepting repeat unit and an arylene co-repeat unit, for example a repeat unit of formula (IV) described below.

Exemplary repeat units include the following:

wherein * denotes the linking points for linking the repeat unit into the polymer chain, and Ak is alkyl, in particular branched or straight chain Ci-io alkyl. Particularly preferred alkyl groups are n-butyl, t-butyl, n-hexyl and n-octyl.

The triplet-accepting unit may be provided as a side-group or end-group of a light-emitting polymer by reacting a compound substituted with one polymerisable group, such as a leaving group capable of participating in a metal-catalysed cross-coupling reaction, such as a halogen or boronic acid or ester, with a leaving group on the polymer.

Alternatively, a side-group may be incorporated into a light-emitting polymer by providing it as a substituent of a monomer as illustrated below:

PG - Polymerisable unit - PG

Triplet-absorbing unit

wherein PG represents a polymerisable group such as a leaving group as described above, or a polymerisable double bond.

In order to increase the probability of TTA and delayed fluorescence as described above, a plurality of triplet-accepting units may be provided in close proximity. For example, two such units may be provided in an optionally substituted unit having the general formula (II):

TAU-Spacer-TAU (Π) wherein "TAU" represents a triplet accepting unit of formula (I) and the spacer is a conjugated or non-conjugated spacer group. The spacer group separates the two triplet- accepting TAU groups, and preferably separates their electronic characteristics (for example the HOMO and LUMO). Depending on the precise nature of the conjugation and orbital overlap, Sp could optionally comprise one or more arylene or heteroarylene groups such as substituted phenyl, biphenyl or fluorene. Alternatively, Sp could optionally comprise a non- conjugated linking group such as alkyl, or another molecular link that does not provide a conjugation path between the TAU groups.

The unit of formula (Ila) may be a separate compound physically mixed with the light- emitting material or it may be bound to the light-emitting material. In the case where the light-emitting material is a polymer, the unit of formula (Ila) may be bound as a main-chain repeat unit, a side group or an end-group as described above.

Alternatively or additionally, the triplet-accepting material may be an oligomer or polymer comprising a repeat unit of formula (lib):

(TAU-Spacer) _m

(lib)

wherein m is at least 2.

Although binding of the triplet-accepting unit to the light-emitting material is described above, it will be appreciated that the triplet-accepting unit may be bound to any other component of the composition, where present, in the same way. For example, the

composition may comprise one or more of a hole transporting and electron transporting material in which case the triplet-accepting unit may be bound to either or both of these units in addition to or as an alternative to binding of the triplet-accepting unit to the light-emitting material. The concentration of the triplet-accepting unit is optionally in the range of at least 0.1 mol % or at least 1 mol%, for example in the range of 0.1-10% or 1 - 10 mol % relative to the light emitting material. A higher concentration of the triplet-accepting material increases the probability of TTA.

In order to increase the probability of TTA, the lifetime of excited state triplets residing on the triplet accepting material is optionally at least 1 microsecond, optionally at least 10 microseconds, optionally at least 100 microseconds. The lifetime of a triplet exciton is its half-life, which may be measured by flash photolysis to measure monomolecular triplet lifetime as described in Handbook of Photochemistry, 2 ^nd Edition, Steven L Murov, Ian Carmichael and Gordon L Hug and references therein, the contents of which are incorporated herein by reference.

It will be appreciated that, unlike phosphorescent dopants, the triplet-accepting material does not provide an energetically favourable pathway for absorbed triplets to undergo radiative decay, and as a result substantially none of the energy of the triplet exciton absorbed by the triplet-accepting material is lost from the triplet-accepting material in the form of

phosphorescent light emission from the triplet-accepting material.

The dynamics of singlet and triplet excitons may be studied using time resolved

electroluminescence as well as quasi-continuous wave (quasi-cw) and time resolved excited state absorption. The density of triplet excitons on a light-emitting material, for example on the polymer backbone of a conjugated light-emitting polymer, may be measured using quasi- cw excited state absorption.

The excited state absorption techniques have been described elsewhere (King, S., Rothe, C. & Monkman, A. Triplet build in and decay of isolated polyspirobifluorene chains in dilute solution. /. Chem. Phys. 121, 10803-10808 (2004), and Dhoot, A.S., Ginger, D.S., Beljonne, D., Shuai, Z. & Greenham, N.C. Triplet formation and decay in conjugated polymer devices. Chemical Physics Letters 360, 195-201 (2002))

For example, the triplet state of polyfluorenes has been well characterised with these techniques with a strong excited state absorption feature peaking at 780nm attributed to the triplet state (King, S., Rothe, C. & Monkman, A. Triplet build in and decay of isolated polyspirobifluorene chains in dilute solution. Chem. Phys. 121, 10803-10808 (2004) and Rothe, C, King, S.M., Dias, F. & Monkman, A.P. Triplet exciton state and related phenomena in the beta-phase of poly(9,9-dioctyl)fluorene. Physical Review B 70, (2004)). Accordingly, probes of triplet population of a polyfluorene may be performed at 780nm, and the skilled person will understand how to modify this probe for other light-emitting materials based on the excited state absorption features of those materials. Figure 4 illustrates the structure of an OLED according to an embodiment of the invention. The OLED comprises a transparent glass or plastic substrate 1, an anode 2, a cathode 4 and a light-emitting layer 3 provided between anode 2 and the cathode 4. Further layers may be located between anode 2 and the cathode, such as charge transporting, charge injecting or charge blocking layers.

Light emitting material

Suitable light-emitting materials for use in layer 3 include small molecule, polymeric and dendrimeric materials, and compositions thereof. Suitable light-emitting polymers for use in layer 3 include poly(arylene vinylenes) such as poly(p-phenylene vinylenes) and polyarylenes such as: polyfluorenes, particularly 2,7-linked 9,9 dialkyl polyfluorenes or 2,7-linked 9,9 diaryl polyfluorenes; polyspirofluorenes, particularly 2,7-linked poly-9,9-spirofluorene; polyindenofluorenes, particularly 2,7-linked polyindenofluorenes; polyphenylenes, particularly alkyl or alkoxy substituted poly-l,4-phenylene. Such polymers as disclosed in, for example, Adv. Mater. 2000 12(23) 1737-1750 and references therein.

A light-emitting polymer may be a light-emitting homopolymer comprising light-emitting repeat units, or it may be a copolymer comprising light-emitting repeat units and further repeat units such as hole transporting and / or electron transporting repeat units as disclosed in, for example, WO 00/55927. Each repeat unit may be provided in a main chain or side chain of the polymer.

Polymers for use as light-emitting materials in devices according to the present invention preferably comprise a repeat unit selected from arylene repeat units as disclosed in, for example, Adv. Mater. 2000 12(23) 1737-1750 and references therein. Exemplary first repeat units include: 1,4-phenylene repeat units as disclosed in J. Appl. Phys. 1996, 79, 934;

fluorene repeat units as disclosed in EP 0842208; indenofluorene repeat units as disclosed in, for example, Macromolecules 2000, 33(6), 2016-2020; and spirofluorene repeat units as disclosed in, for example EP 0707020. Each of these repeat units is optionally substituted. Examples of substituents include solubilising groups such as C _1-2 o alkyl or alkoxy; electron withdrawing groups such as fluorine, nitro or cyano; and substituents for increasing glass transition temperature (Tg) of the polymer. Particularly preferred polymers comprise optionally substituted, 2,7-linked fluorenes, most preferably repeat units of formula IV:

(IV)

wherein R ¹ and R ² are independently H or a substituent and wherein R ¹ and R ² may be linked to form a ring. R ¹ and R ² are preferably selected from the group consisting of hydrogen; optionally substituted alkyl wherein one or more non-adjacent C atoms may be replaced with O, S, N, C=0 and -COO-; optionally substituted aryl or heteroaryl; and

1 2 optionally substituted arylalkyl or heteroarylalkyl. More preferably, at least one of R and R comprises an optionally substituted alkyl, for example Q-C20 alkyl, or aryl group.

"Aryl" and "heteroaryl" as used herein includes both fused and unfused aryl and heteroaryl groups respectively.

Optionally, fluorene repeat units are present in an amount of at least 50 mol %.

In the case where R ¹ or R ² comprises aryl or heteroaryl, a preferred aryl or heteroaryl group is phenyl, and preferred optional substituents include alkyl groups wherein one or more non- adjacent C atoms may be replaced with O, S, N, C=0 and -COO-.

Optional substituents for the fluorene unit, other than substituents R ¹ and R ² , are preferably selected from the group consisting of alkyl wherein one or more non-adjacent C atoms may be replaced with O, S, N, C=0 and -COO-, optionally substituted aryl, optionally substituted heteroaryl, alkoxy, alkylthio, fluorine, cyano and arylalkyl.

Preferably, the polymer comprises an arylene repeat unit as described above and an arylamine repeat unit, in particular a repeat unit V:

(V) 1 2.

wherein Ar and Ar are optionally substituted aryl or heteroaryl groups, n is greater than or equal to 1, preferably 1 or 2, and R is H or a substituent, preferably a substituent. R is preferably alkyl or aryl or heteroaryl, most preferably aryl or heteroaryl. Any of the aryl or heteroaryl groups in the unit of formula 1, including the case where R is aryl or heteroaryl, may be substituted, and in one embodiment Ar ¹ , Ar ² and R are each optionally substituted phenyl. . Preferred substituents are selected from alkyl wherein one or more non-adjacent C atoms may be replaced with O, S, N, C=0 and -COO-, optionally substituted aryl, optionally substituted heteroaryl, alkoxy, alkylthio, fluorine, cyano and arylalkyl. Preferred substituents include alkyl and alkoxy groups. Any of the aryl or heteroaryl groups in the repeat unit of Formula 1 may be linked by a direct bond or a divalent linking atom or group. Preferred divalent linking atoms and groups include 0, S; substituted N; and substituted C.

Particularly preferred units satisfying Formula 1 include units of Formulae 1-3:

1 2 3 wherein Ar ¹ and Ar ² are as defined above; and Ar ³ is optionally substituted aryl or heteroaryl. Where present, preferred substituents for Ar ³ include alkyl and alkoxy groups.

The arylamine repeat units are preferably present in an amount up to 30 mol , preferably up to 20 mol%. These percentages apply to the total number of arylamine units present in the polymer in the case where more than one type of repeat unit of formula V is used. Repeat units of formula (V) may provide one or more of hole transporting functionality and light- emitting functionality.

The polymer may comprise heteroarylene repeat units for charge transport or emission.

Binding a triplet-accepting unit to the light-emitting material may result in more efficient triplet absorption as compared to mixing of a triplet-accepting material with the light-emitting material because this binding may provide intramolecular triplet absorption pathways unavailable to a corresponding mixed system.

Moreover, binding may be beneficial for processing reasons. For example, if the triplet- accepting unit has low solubility then binding it to a soluble light-emitting material, in particular a light-emitting polymer, allows the triplet-accepting unit to be carried in solution by the light-emitting material, enabling device fabrication using solution processing techniques. Furthermore, if the triplet-accepting unit is a relatively volatile material, such as stilbene or a derivative thereof, then the risk of evaporation of the triplet accepting material during device fabrication is eliminated. This is a particular issue in the case of OLEDs formed using solution processing methods because light-emitting layers formed by deposition of a solution are typically heated as part of the device fabrication process (for example, to evaporate the solvent), which increases the likelihood of evaporation of volatile triplet- accepting units. Finally, binding the triplet accepting unit to the light-emitting material may prevent phase separation effects in solution-processed devices that may be detrimental to device performance.

Where the light-emitting material is a conjugated polymer comprising light-emitting repeat units and further repeat units, for example light-emitting amine repeat units of formula (V) and fluorene repeat units of formula (IV), conjugation of the triplet-accepting unit into the polymer main chain (for example by conjugation with fluorene repeat units) may reduce the energy level of the triplet-accepting unit, thus increasing the energetic favourability of triplet exciton transfer from the emitter unit to the triplet-accepting unit. This reduction in Ti energy level of the triplet-accepting unit may also enable use of the triplet-accepting unit with light-emitting materials with j levels that are too low for use with a triplet-accepting unit that is not conjugated in this way.

Preferred methods for preparation of conjugated light-emitting polymers comprise a "metal insertion" wherein the metal atom of a metal complex catalyst is inserted between an aryl or heteroaryl group and a leaving group of a monomer. Exemplary metal insertion methods are Suzuki polymerisation as described in, for example, WO 00/53656 and Yamamoto polymerisation as described in, for example, T. Yamamoto, "Electrically Conducting And Thermally Stable π - Conjugated Poiy(arylene)s Prepared by Organometallic Processes", Progress in Polymer Science 1993, 17, 1153-1205. In the case of Yamamoto polymerisation, a nickel complex catalyst is used; in the case of Suzuki polymerisation, a palladium complex catalyst is used.

For example, in the synthesis of a linear polymer by Yamamoto polymerisation, a monomer having two reactive halogen groups is used. Similarly, according to the method of Suzuki polymerisation, at least one reactive group is a boron derivative group such as a boronic acid or boronic ester and the other reactive group is a halogen. Preferred halogens are chlorine, bromine and iodine, most preferably bromine.

It will therefore be appreciated that repeat units illustrated throughout this application may be derived from a monomer carrying suitable leaving groups. Likewise, an end group or side group may be bound to the polymer by reaction of a suitable leaving group.

Suzuki polymerisation may be used to prepare regioregular, block and random copolymers. In particular, homopolymers or random copolymers may be prepared when one reactive group is a halogen and the other reactive group is a boron derivative group. Alternatively, block or regioregular, in particular AB, copolymers may be prepared when both reactive groups of a first monomer are boron and both reactive groups of a second monomer are halogen.

As alternatives to halides, other leaving groups capable of participating in metal insertion include groups include tosylate, mesylate and triflate.

Light-emitting layer 3 may consist of the light-emitting polymer and the triplet accepting unit alone, alone or may comprise these materials in combination with one or more further materials. In particular, the light-emitting polymer may be blended with hole and / or electron transporting materials or alternatively may be covalently bound to hole and / or electron transporting materials as disclosed in for example, WO 99/48160.

Light-emitting copolymers may comprise a light-emitting region and at least one of a hole transporting region and an electron transporting region as disclosed in, for example, WO 00/55927 and US 6353083. If only one of a hole transporting region and electron transporting region is provided then the electroluminescent region may also provide the other of hole transport and electron transport functionality - for example, an amine unit as described above may provide both hole transport and light-emission functionality. A light- emitting copolymer comprising light-emitting repeat units and one or both of a hole transporting repeat units and electron transporting repeat units may provide said units in a polymer main-chain, as per US 6353083, or in polymer side-groups pendant from the polymer backbone.

The light-emitting polymer may emit light of any colour provided that its Si and energy levels relative to the triplet-accepting unit are as described above, however the light-emitting polymer is preferably a blue light-emitting polymer, in particular a material having photoluminescent light emission with a peak wavelength in the range of from 400 to 500 nm, preferably 430 to 500 nm.

Light-emitting layer layer 3 may be patterned or unpatterned. A device comprising an unpatterned layer may be used an illumination source, for example. A white light emitting device is particularly suitable for this purpose. A device comprising a patterned layer may be, for example, an active matrix display or a passive matrix display. In the case of an active matrix display, a patterned electroluminescent layer is typically used in combination with a patterned anode layer and an unpatterned cathode. In the case of a passive matrix display, the anode layer is formed of parallel stripes of anode material, and parallel stripes of electroluminescent material and cathode material arranged perpendicular to the anode material wherein the stripes of electroluminescent material and cathode material are typically separated by stripes of insulating material ("cathode separators") formed by photolithography.

Hole injection layers

A conductive hole injection layer, which may be formed from a conductive organic or inorganic material, may be provided between the anode 2 and the electroluminescent layer 3 to assist hole injection from the anode into the layer or layers of semiconducting polymer. Examples of doped organic hole injection materials include optionally substituted, doped poly(ethylene dioxythiophene) (PEDT), in particular PEDT doped with a charge -balancing polyacid such as polystyrene sulfonate (PSS) as disclosed in EP 0901176 and EP 0947123, polyacrylic acid or a fluorinated sulfonic acid, for example Nafion ®; polyaniline as disclosed in US 5723873 and US 5798170; and optionally substituted polythiophene or poly(thienothiophene). Examples of conductive inorganic materials include transition metal oxides such as VOx MoOx and RuOx as disclosed in Journal of Physics D: Applied Physics (1996), 29(11), 2750-2753.

Charge transporting layers

A hole transporting layer may be provided between the anode and the electroluminescent layer. Likewise, an electron transporting layer may be provided between the cathode and the electroluminescent layer.

Similarly, an electron blocking layer may be provided between the anode and the

electroluminescent layer and a hole blocking layer may be provided between the cathode and the electroluminescent layer. Transporting and blocking layers may be used in combination. Depending on its HOMO and LUMO levels, a single layer may both transport one of holes and electrons and block the other of holes and electrons.

If present, a hole transporting layer located between anode 2 and electroluminescent layer 3 preferably has a HOMO level of less than or equal to 5.5 eV, more preferably around 4.8-5.5 eV. HOMO levels may be measured by cyclic voltammetry, for example.

If present, an electron transporting layer located between electroluminescent layer 3 and cathode 4 preferably has a LUMO level of around 3-3.5 eV. For example, a layer of a silicon monoxide or silicon dioxide or other thin dielectric layer having thickness in the range of 0.2-2nm is provided between electroluminescent layer 3 and layer 4.

Polymers for use as charge transporting materials may comprise arylene units, such as fluorene units of formula (IV) and other units described above.

A hole-transporting polymer may comprise arylamine repeat units, in particular repeat units of formula (V), such as repeat units of formulae 1-3, described above. This polymer may be a homopolymer or it may be a copolymer comprising arylene repeat units in an amount up to 95 mol %, preferably up to 70 mol %. These percentages apply to the total number of arylamine units present in the polymer in the case where more than one type of repeat unit of formula (V) is used.

Charge transporting units may be provided in a polymer main-chain or polymer side-chain. Cathode

Cathode 4 is selected from materials that have a workfunction allowing injection of electrons into the electroluminescent layer. Other factors influence the selection of the cathode such as the possibility of adverse interactions between the cathode and the electroluminescent material. The cathode may consist of a single material such as a layer of aluminium.

Alternatively, it may comprise a plurality of metals, for example a bilayer of a low

workfunction material and a high workfunction material such as calcium and aluminium as disclosed in WO 98/10621; elemental barium as disclosed in WO 98/57381, Appl. Phys. Lett. 2002, 81(4), 634 and WO 02/84759; or a thin layer of metal compound, in particular an oxide or fluoride of an alkali or alkali earth metal, to assist electron injection, for example lithium fluoride as disclosed in WO 00/48258; barium fluoride as disclosed in Appl. Phys. Lett. 2001, 79(5), 2001; and barium oxide. In order to provide efficient injection of electrons into the device, the cathode preferably has a workfunction of less than 3.5 eV, more preferably less than 3.2 eV, most preferably less than 3 eV. Work functions of metals can be found in, for example, Michaelson, J. Appl. Phys. 48(11), 4729, 1977.

The cathode may be opaque or transparent. Transparent cathodes are particularly

advantageous for active matrix devices because emission through a transparent anode in such devices is at least partially blocked by drive circuitry located underneath the emissive pixels. A transparent cathode will comprises a layer of an electron injecting material that is sufficiently thin to be transparent. Typically, the lateral conductivity of this layer will be low as a result of its thinness. In this case, the layer of electron injecting material is used in combination with a thicker layer of transparent conducting material such as indium tin oxide.

It will be appreciated that a transparent cathode device need not have a transparent anode (unless, of course, a fully transparent device is desired), and so the transparent anode used for bottom-emitting devices may be replaced or supplemented with a layer of reflective material such as a layer of aluminium. Examples of transparent cathode devices are disclosed in, for example, GB 2348316.

Encapsulation

Optical devices tend to be sensitive to moisture and oxygen. Accordingly, the substrate preferably has good barrier properties for prevention of ingress of moisture and oxygen into the device. The substrate is commonly glass, however alternative substrates may be used, in particular where flexibility of the device is desirable. For example, the substrate may comprise a plastic as in US 6268695 which discloses a substrate of alternating plastic and barrier layers or a laminate of thin glass and plastic as disclosed in EP 0949850.

The device is preferably encapsulated with an encapsulant (not shown) to prevent ingress of moisture and oxygen. Suitable encapsulants include a sheet of glass, films having suitable barrier properties such as silicon dioxide, silicon monoxide, silicon nitride or alternating stacks of polymer and dielectric as disclosed in, for example, WO 01/81649 or an airtight container as disclosed in, for example, WO 01/19142. In the case of a transparent cathode device, a transparent encapsulating layer such as silicon monoxide or silicon dioxide may be deposited to micron levels of thickness, although in one preferred embodiment the thickness of such a layer is in the range of 20-300 nm. A getter material for absorption of any atmospheric moisture and / or oxygen that may permeate through the substrate or encapsulant may be disposed between the substrate and the encapsulant.

Solution processing

Light-emitting layer 3 may be deposited by any process, including vacuum evaporation and deposition from a solution in a solvent. In the case where the light emitting layer comprises a polyarylene, such as a polyfluorene, suitable solvents for solution deposition include mono- or poly-alkylbenzenes such as toluene and xylene. Particularly preferred solution deposition techniques including printing and coating techniques, preferably spin-coating and inkjet printing.

Spin-coating is particularly suitable for devices wherein patterning of the electroluminescent material is unnecessary - for example for lighting applications or simple monochrome segmented displays.

Inkjet printing is particularly suitable for high information content displays, in particular full colour displays. A device may be inkjet printed by providing a patterned layer over the first electrode and defining wells for printing of one colour (in the case of a monochrome device) or multiple colours (in the case of a multicolour, in particular full colour device). The patterned layer is typically a layer of photoresist that is patterned to define wells as described in, for example, EP 0880303. As an alternative to wells, the ink may be printed into channels defined within a patterned layer. In particular, the photoresist may be patterned to form channels which, unlike wells, extend over a plurality of pixels and which may be closed or open at the channel ends.

Other solution deposition techniques include dip-coating, roll printing and screen printing.

If multiple layers of an OLED are formed by solution processing then the skilled person will be aware of techniques to prevent intermixing of adjacent layers, for example by crosslinking of one layer before deposition of a subsequent layer or selection of materials for adjacent layers such that the material from which the first of these layers is formed is not soluble in the solvent used to deposit the second layer.

Composition Example 1

Anthanthrene compound 1 was prepared according to the following synthetic method, starting from commercially available anthanthrene:

Compound 1 was blended with a polymer comprising fluorene repeat units of formula (V) and light-emitting amine repeat units of formula (IV).

Device Example 1

A device having the following structure was formed:

ITO / HIL / HTL / EL / MF / Al

wherein ITO represents an indium-tin oxide anode; HIL is a 35 nm hole-injection layer; HTL is a 15 nm hole transport layer of a polymer of formula (IV); EL is an 70 nm

electroluminescent layer containing the light-emitting polymer of formula (V) blended with a triplet accepting material (DPVBi, 1% mol ratio) of formula (VI) (a control device without DPVBi was also made for comparison); MF is a metal fluoride; and the bilayer of MF / Al forms a cathode for the device. The HIL, HTL and EL layers were deposited by spin-coating or inkjet printing the composition from solution and evaporating the solvent.

DPVBi has a triplet level below that of the polyfluorene triplet (Chen, P., et al. Appl. Phys. Lett. 91:023505, 2007; Schwartz, G. et al. Appl. Phys. Lett. 89:083509, 2006) and has a high singlet energy (3.2eV) compared to the luminescent polymer, ensuring that the emissive singlet states are not affected by the triplet accepting material.

The dynamics of the singlet and triplet excitons were measured by time resolved electroluminescence, quasi-cw, and time-resolved excited state absorbtion techniques. The polyfluorene triplet state was monitored using the previously mentioned excited state absorption feature at 780nm, modulating the current to the device, and measuring absorption with a lock-in amplifier. Fig. 5 shows external quantum efficiency of a Device Example l_without (boxes) and with (circles) the addition of the triplet accepting material. The presence of the triplet accepting material did not change the electroluminescence spectrum of the device.

Fig. 6. shows the quasi-cw current induced excited state absorption curves of Device Example 1 without (squares) and with (solid circles) the addition of the triplet accepting material. These curves indicate the density of triplet excitons on the polymer backbone. Also shown is the Device Example 1 driven to half the initial luminance (diamonds).

Fig. 7a shows the time resolved electroluminescence during the turn off of Device Example 1. Following an initial RC decay, there was a residual electroluminescent signal accounting for about 30% of the total original electroluminescence having a time scale of a few microseconds, which is attributed to TTA. Electroluminescence turn-off of Device Example 1 (open squares) compared with the time resolved transient triplet absorption (solid squares) and its square (solid circles). The dotted lines are of the same slope. Also shown is the effect on the electroluminescence turn off when a reverse bias pulse of 10V for 200 ns duration is applied to the device 250 ns after the device current is switched off (open circles) in order to distinguish TTA from recombination of trapped charge. The data of this figure show that the residual decay of electroluminescence is due to bimolecular triplet-triplet annihilation reactions (TTA) resulting in emissive singlet excitons.

Fig. 7b shows Electroluminescence turn off transients for an undriven device (T100) and devices driven to different relative luminance (e.g., T90 is driven to 90% of starting luminance). Also shown in the inset is the normalized luminance decay of the device (solid squares) compared to the normalized contribution that TTA singlets make to the device efficiency (open circles).

Fig. 8 shows the decay of the device luminance (upper panel) with time and the change in efficiency of the device with time (lower) for a standard device (solid line) and a device containing the triplet quenching additive (dashed line). The devices were both driven from a starting luminance of 5000 cd m ^'2 .

Without thereby being limited by theory, a significant proportion of the device electroluminescence originates from the generation of emissive singlet excitons from a triplet-triplet annihilation process. As a result of the efficient quenching of the triplet excitons by the defect sites generated in the polymer film during driving, this boost to the device efficiency is lost early on in the device lifetime and is a significant contribution to the rapid initial decay often seen in high efficiency fluorescent OLED devices. The lifetime of the device is significantly enhanced using a triplet quenching additive. Using this approach, a >3_ improvement in the device half-life (T50) and >5 improvement in the initial decay (T90) were realized.

Device Example 2

A further device was prepared substantially as described in Device Example 1 except that the triplet-accepting material was 9,10-diphenylanthracene. Fig. 9a shows the delayed emission, backbone triplet density and square of the backbone triplet density for a device without triplet quencher. The straight lines are a guide to the eye showing that delayed emission is proportional to the square of the backbone triplet density. Fig. 9b shows the delayed emission, triplet density and square of the triplet density for a device containing 9,10- diphenylanthracene as triplet-accepting material.

Example 3

A yet further example was prepared in which the triplet-accepting material (an anthracene) was provided within the backbone of the light emitting polymer in the form of an anthracene - fluorene random copolymer comprising 50 mol% of anthracene and fluorene monomers. Fig. 10 shows delayed fluorescence obtained using this material.

Although the present invention has been described in terms of specific exemplary

embodiments, it will be appreciated that various modifications, alterations and/or

combinations of features disclosed herein will be apparent to those skilled in the art without departing from the scope of the invention as set forth in the following claims.