ライフサイエンスコーパス: triplet

1 junctions of tubules likely to reinforce the triplet.

2 Magnetic data show this complex to be a triplet.

3 for the transition into formally independent triplets.

4 d by separation into weakly bound, localized triplets.

5 to two consecutive non-canonical A*G-C base triplets.

6 photoprotective quenching of harmful (B)Chl triplets.

7 red triplets within long stretches of d(CGA) triplets.

8 nt Cl(*) radical migration forms a localized triplet 1,3-diradical intermediate that, after intersyst

9 leton pregnancies, 51 were twins, and 2 were triplets (304 total fetuses).

10 nalizing non-toxic silicon nanocrystals with triplet-accepting anthracene ligands.

11 t exciton transfer from silicon to molecular triplet acceptors can critically enable new technologies

12 er favour or prohibit charge transfer as the triplet acceptors.

13 thods, RETrace achieved higher accuracy (88% triplet accuracy from an ex vivo HCT116 tree) at a highe

14 haracterize these transient intermediates as triplet adducts of Rh(2).

15 y gaps of J and 3J separate a singlet from a triplet and a singlet from a quintet, respectively.

16 d 1201 cm(-1) characteristic of the collagen triplet and indicative of fibrosis.

17 ability of the PheB24-PheB25-TyrB26 aromatic triplet and opens a new direction for therapeutic insuli

18 spin-dependent inter-system crossing between triplet and singlet manifolds, indicating that optically

19 by changing the 5'-nucleobase of the d(CGA) triplet and the frequency and position of the altered tr

20 ted with neurodegeneration revealed that the triplets and the affected offspring are heterozygous car

21 We analyzed 2973 triplet APU samples from 1255 patients.

22 Results show that correlations among triplets are higher during correct choices with respect

23 early demonstrating the relationship between triplet aromaticity and singlet-triplet energy gap, conf

24 isms underlying the stability of microtubule triplets, as well as centriole architectural integrity r

25 tRNAs universally carry a CCA nucleotide triplet at their 3'-ends.

26 Twenty-eight variant positions, and a triplet ATT codon (Ile) insertion within ATP synthase su

27 very and tolerance profile of doublet versus triplet bortezomib-based regimens in patients with initi

28 rotonation, including whether the singlet or triplet carbene is formed, are probed.

29 ndent interplay between emissive singlet and triplet charge-transfer states and amide-localized tripl

30 y back transfer, sensitizer aggregation, and triplet-charge annihilation.

31 investigated the addition of panitumumab to triplet chemotherapy with fluorouracil/folinic acid, oxa

32 rk" exciton, an electron-hole pair in a spin-triplet configuration.

33 gets a linear combination of the singlet and triplet configurations involving the HOMO and LUMO rathe

34 to show how flies combine local pairwise and triplet correlations to reduce variability in motion est

35 This independent modulation of singlet and triplet decay rates is highly desirable for the design o

36 For the first time, triplet decorrelation through intramolecular triplet dif

37 triplet decorrelation through intramolecular triplet diffusion was observed following SF.

38 t oxygen obtained from photosensitization of triplet dioxygen is shown to react with an alkene surfac

39 t dissociation at optimal driving forces for triplet dissociation.

40 with very low surface trap densities as the triplet donor and polyacenes which either favour or proh

41 Hence, triplet dynamics are conventionally controlled through h

42 e demonstrate that it is possible to control triplet dynamics by coupling organic molecules to lantha

43 opy and modelling to unravel the singlet and triplet dynamics.

44 may consequently consist of both singlet and triplet emission.

45 ts in the design and realization of tailored triplet emitters with nonconventional elements.

46 on (enhanced use of photon energy and larger triplet energies for coupling with common absorbers) mot

47 megaB97XD*) was used to rigorously calculate triplet energies, while a systematic analysis of electro

48 theoretical model, indicated a large singlet-triplet energy gap (DeltaE(S-T) = -45 kcal/mol), a high

49 ship between triplet aromaticity and singlet-triplet energy gap, confirming this novel strategy for m

50 The precisely controlled triplet energy levels of the quantum dot photocatalysts

51 Mechanistic experiments revealed that triplet energy sensitization of a Cu-bound radical precu

52 rbit coupling(9-11) or tuning of the singlet-triplet energy splitting(12,13) via molecular design.

53 cal and electronic properties, small singlet-triplet energy splitting, narrow emission line widths, a

54 likely due to elevation of the zeta-carotene triplet energy state above that of BChl a These findings

55 ements, a direct proxy for the efficiency of triplet energy transfer (TET), as well as transient abso

56 The mechanisms of triplet energy transfer across the inorganic nanocrystal

57 nneling-to-hopping transition for long-range triplet energy transfer between nanocrystal light absorb

58 motor pillars confirms efficient triplet-to-triplet energy transfer between the porphyrin linkers an

59 his class of oximes can be harnessed via the triplet energy transfer from a commercially available ir

60 t absorption spectroscopy is used to confirm triplet energy transfer from CdSe to transmitter, and th

61 the excess vibrational energy available from triplet energy transfer leads to hot and nonstatistical

62 numerous photoredox catalytic processes and triplet energy transfer.

63 are consistent with a reaction course via a triplet enone intermediate and the formation of a 1,4-di

64 sly, but proceeds through spin-mixing in the triplet exciplex.

65 hange and hyperfine interactions in the spin triplet exciplex.

66 ctive conformations and the participation of triplet exciplexes.

67 ergo efficient upconversion via a lanthanide-triplet excitation fusion process: this process enables

68 sor structure followed by dimerization after triplet excitation.

69 t the co-existence of efficient ISC and long triplet excited lifetime in a heavy atom-free bodipy hel

70 and aromaticity upon excitation to the first triplet excited state (T(1)).

71 ransfer (PeT) from a thiolate to Cy in their triplet excited state and then triplet-to-singlet inters

72 Triplet excited state chemistry has enabled a range of i

73 uasi-2D nanoplatelets, as photocatalysts for triplet excited state chemistry.

74 ing fluorophores, photoswitching agents, and triplet excited state quenchers for single-molecule and

75 the reaction proceeds via cyclization in the triplet excited state to yield a 1,4-diradical; intersys

76 y, suggesting an intersystem crossing to the triplet excited state with subsequent phosphorescent dec

77 suggesting that bond scission occurs from a triplet excited state.

78 mparted due to the delocalized nature of the triplet excited state.

79 so derivatives, likely via the production of triplet excited states ((3)NOM*) and HO(*).

80 Besides the SOC induced ISC pathway, triplet excited states are also realised in organic chro

81 insights into the diverse pathways to access triplet excited states in organic chromophores.

82 deep red to near-IR emission involving their triplet excited states in the solid state and in PMMA fi

83 atial restriction efficiently rigidified the triplet excited states of carbon dots from non-radiative

84 prove beneficial for researchers to achieve triplet excited states of organic chromophores for numer

85 ecades, exploring the pathways to access the triplet excited states of organic chromophores has been

86 relative energies of the lowest singlet and triplet excited states, enhancing the yield of triplet-t

87 ly on the energies of the lowest singlet and triplet excited states.

88 strated that QDs impart stereoselectivity to triplet excited-state [2 + 2] cycloaddition reactions of

89 The analysis revealed that the neutral triplet exciton is substantially more delocalized than t

90 Triplet exciton states of the molecules can undergo ener

91 range tunneling to long-range hopping during triplet exciton transfer from CdSe nanocrystals to anthr

92 Photoexciting these structures drives spin-triplet exciton transfer from silicon to anthracene thro

93 Our demonstration of spin-triplet exciton transfer from silicon to molecular tripl

94 addition, the delocalization of the neutral triplet exciton was also determined in the oligomers and

95 iconductor nanocrystals interfaced with spin-triplet exciton-accepting organic molecules have emerged

96 Dynamic triplet-exciton behaviours including thermally activated

97 Molecular triplet excitons (bound electron-hole pairs) are 'dark s

98 on, a localized buildup of slow-decaying(14) triplet excitons and charges(15) gradually reduces the b

99 The formation of two triplet excitons at the cost of one photon via singlet e

100 Furthermore, we demonstrate that the triplet excitons generated in the lanthanide nanoparticl

101 iency on SWCNT structure suggests that (7,6) triplet excitons have an energy near 970 meV.

102 The generation, control and transfer of triplet excitons in molecular and hybrid systems is of g

103 phenomenon, we study charge separation from triplet excitons in polycrystalline pentacene using an e

104 y conversion events that ultimately fuse two triplet excitons into a singlet exciton.

105 is via the efficient extraction of the dark triplet excitons into quantum dots (QDs) where they can

106 uorescent materials that efficiently convert triplet excitons into singlets through reverse intersyst

107 nerated singlet excitons can be converted to triplet excitons on sub-10-picosecond timescales with un

108 -scale fluorescence arising from upconverted triplet excitons that are directly created through energ

109 ause singlet fission produces two low-energy triplet excitons that have been unexpectedly difficult t

110 ch provides sufficient statistical space for triplet excitons to separate and avoid annihilation-and

111 cess of splitting a singlet exciton into two triplet excitons, has been proposed as a mechanism for i

112 n, converting singlet excitons into pairs of triplet excitons, have potential as photovoltaic materia

113 a function of driving force for singlet and triplet excitons, including inverted regimes for the dis

114 singlet exciton is roughly isoergic with two triplet excitons, the limiting step is the triplet-tripl

115 These results provide a new way to control triplet excitons, which is essential for many fields of

116 o achieve luminescent harvesting of the dark triplet excitons.

117 of unstructured proteins, the micelles favor triplet formation.

118 nglet fission-that is, the generation of two triplets from a lone singlet state-has recently resurfac

119 up to 1100 nm and almost degenerate singlet-triplet ground states with weak antiferromagnetic intera

120 ree survival was numerically improved in the triplet group-16.0 months-compared with 10.3 months in t

121 ed by a nine-fold arrangement of microtubule triplets held together by an inner protein scaffold.

122 nes such as butadiynylcyclopropenylidene and triplet heptatriynylidene, thus offering a versatile str

123 tition per se, and underscores that treating triplets in the sequence independently and averaging acr

124 ability of ribosomes to accurately recognize triplet interactions between codons on mRNAs and anticod

125 nitrene formation proceeding via a transient triplet intermediate before reaching a planar singlet sp

126 t increase the chance of finding the singlet-triplet intersection seam.

127 the genetic code; disseminating nucleic acid triplets into correct amino acid identity.

128 minant structure in the wild type exhibits a triplet involving the unpaired nucleotide U40 and the ba

129 the nature of the excited state (singlet vs triplet) is dependent on aromatic substitution.

130 centrioles lacking a full set of microtubule triplets, its overactivity results in over-elongated and

131 the spin-zero ground state and the spin-one triplet levels(8).

132 The long triplet lifetime ensures high-efficiency singlet oxygen

133 he increase in entropy, thus lengthening the triplet lifetime in longer oligomers.

134 ctroscopy in solution reveals much prolonged triplet lifetime of PTC-1(2H) relative to monomer refere

135 ith the rate constants estimated from the BP triplet lifetimes.

136 his molecule has an exceptionally long-lived triplet LMCT excited state (tau = 350 mus), featuring hi

137 A CUG triplet located in the 5' leader of POLG messenger RNA (

138 s CUG directs translation of a conserved 260-triplet-long overlapping open reading frame (ORF), which

139 Accessing the triplet manifold in pai-conjugated systems would also in

140 o that of the nitrenium ion, suggestive of a triplet mechanism.

141 the context of both the radical pair and the triplet mechanisms of spin polarization.

142 igand stretching vibrational wavepacket on a triplet metal-centered ((3)MC) excited state surface.

143 Direct singlet-to-triplet metal-to-ligand charge transfer (MLCT) transitio

144 et of non-tubulin components attached to the triplet microtubule (MT), many are at the junctions of t

145 While the BB is composed of triplet microtubules (TMTs), the axoneme is composed of

146 system crossing leads to the population of a triplet minimum of the thietane intermediate in as short

147 ific differences in the interaction of their triplet motifs determine the profound differences in KCN

148 th the PD-1-blocking antibody pembrolizumab (triplet; n = 60) or placebo (doublet; n = 60).

149 radical chemistry (intersystem crossing with triplet O(2)) does not seem to be involved in O(2) activ

150 RNF43 activity requires phosphorylation at a triplet of conserved serines.

151 explore how hypophosphorylation of Cx43 at a triplet of serine residues (S325/S328/S330) in the regul

152 the genetic code in messenger RNA (mRNA) as triplets of nucleotides in a single reading frame.

153 the option to skip bases between the target triplets of otherwise adjacent fingers in each zinc-fing

154 loss of m(5) C impacts the decoding of some triplets of these two amino acids, leading to reduced tr

155 omega(flap) = +/-44 deg) and C(2v)-symmetric triplet (omega(flap) = 0 deg) stem from nonclassical ele

156 Higher-order patterns, such as triplet or triangle motifs, have been tied to cooperativ

157 erlapping such as competing structures, base triplets, or other 3D non-antiparallel interactions.

158 functionalized derivative leads to efficient triplet pair separation, giving rise to an overall tripl

159 We analyze correlated-triplet-pair (TT) singlet-fission intermediates toward t

160 et-pair state, which we attribute to singlet/triplet-pair interconversion at these sites.

161 omophores about the molecular axis following triplet-pair separation contributes to the increase in e

162 This work demonstrates that a real, emissive triplet-pair state acts as an intermediate in both singl

163 are believed to be mediated by a biexcitonic triplet-pair state, (1)(TT).

164 inglet states matches that of the correlated triplet-pair state, which we attribute to singlet/triple

165 Combined with existing data that indicate triplet pairing in UTe(2), the presence of chiral states

166 Nevertheless, the mechanism of spin-triplet pairing is much less understood than that of spi

167 However, triplet pairing is rare in solid-state systems and has n

168 An interesting manifestation of triplet pairing is the chiral p-wave state, which is top

169 f beta-Bi(2)Pd and is consistent with a spin-triplet pairing symmetry.

170 totype carbenes with distinct multiplicities-triplet pentadiynylidene (HCCCCCH) and singlet ethynylcy

171 ofuran-2-carboxylates using rose bengal as a triplet photosensitizer at ambient temperature.

172 ), leading to unprecedented performance as a triplet photosensitizer for PDT.

173 Intersystem crossing (ISC) of triplet photosensitizers is a vital process for fundamen

174 The most popular triplet photosensitizers, metal complexes and organic ch

175 Such photoreactions are triggered by triplet photosensitizers, which absorb visible-light pho

176 photostability enhance their performance as triplet photosensitizers.

177 (hole); the separation rates for singlet and triplet polaron pairs: k(S,s) = (44.59 +/- 0.01) MHz, k(

178 Triplet populations evolve and relax much faster in P3HS

179 x10(5) m(-1) cm(-1) at 630 nm), satisfactory triplet quantum yield (Phi(T) =52 %), and long-lived tri

180 propose a module consisting of spin singlet-triplet qubits and single microwave photons.

181 we explore an important resource for singlet-triplet qubits: a transverse sweet spot (TSS) that enabl

182 by an order of magnitude, while the rate of triplet recombination is approximately the same.

183 ed to assess the efficacy and safety of this triplet regimen in patients with relapsed or refractory

184 The VRd triplet regimen remains the standard of care for inducti

185 I are fragile, and indication for doublet or triplet regimen should be adapted to frailty.

186 combination with dexamethasone as well as in triplet regimens with additional classes of drugs.

187 Triplet repeat diseases (TRDs) are caused by pathogenic

188 a is a unique endonuclease that can initiate triplet repeat DNA expansions.

189 inhibition as an attractive therapy in some triplet repeat expansion diseases.

190 In addition to MutLgamma, triplet repeat expansion involves the mismatch recogniti

191 In humans, triplet repeat expansion is the molecular basis for ~40

192 of MutL proteins that has been implicated in triplet repeat expansion, but its action in this deleter

193 into an innovative regulatory mechanism for triplet repeat expansions.

194 HDAC3 function in the same pathway to drive triplet repeat expansions.

195 the stability and versatility of the d(CGA) triplet repeat motif and provides constraints for using

196 The d(CGA) triplet repeat motif is structurally dynamic and can tra

197 elocalization to the NPC of expanded CAG/CTG triplet repeats.

198 p process, resulting in a median loss of ~60 triplet repeats.

199 ocess, injecting entanglement in the form of triplet resonating valence bonds into the ordered ferrom

200 local moments and conduction electrons, from triplet resonating valence bonds to Kondo-entangled sing

201 In this work, we investigate the triplet-sensitized photodegradation of cysteine sulfinic

202 (anti-head-to-tail), or exclusively 5 in the triplet-sensitized photoreaction, in the presence of ben

203 em catalysis by reacting with the oxime as a triplet sensitizer in the first catalytic cycle and a re

204 Our analysis indicates that triplet sensitizers act as one-electron oxidants on the

205 her oxidized to SO(4)(2-) in the presence of triplet sensitizers and oxygen.

206 TT) singlet-fission intermediates toward two-triplet separation (T...T) using spin-state-averaged den

207 A repeating triplet-sequence ABA- of non-overlapping brief tones, A

208 d across noninvasive studies of streaming of triplets; show percept-related changes in frontoparietal

209 otion percepts incorporate both pairwise and triplet spatiotemporal correlations that could theoretic

210 owever, even in fibers, the formation of the triplet species increases with increasing peptide/porphy

211 a structure of (.) OH...OP(.) , for which a triplet spin multiplicity with a binding energy of -3.20

212 outer-sphere reductive elimination step via triplet spin state from the Ni(III) intermediates.

213 ealed that access to high spin states (e.g., triplet spin state tetrahedral Ni(II) species) is critic

214 They are characterized by singlet-triplet spin-flip inelastic excitations with an effectiv

215 proximal position with F shifts the singlet-triplet splitting by +4.5 +/- 0.4 kcal mol(-1) from orth

216 harmonic vibrational frequencies and singlet-triplet splittings are computed using the benchmarked fu

217 The lowest triplet state (T(1) , 1.89 eV) is localized on the TBP a

218 quantum yield (Phi(T) =52 %), and long-lived triplet state (tau(T) =492 mus), leading to unprecedente

219 o transmitter, and the formation of a bridge triplet state as an intermediate for the hopping mechani

220 essarily reliable for determining the lowest triplet state energy level.

221 also to predict their reactivities based on triplet state energy transfer and transition state energ

222 e rate constant for charge transfer from the triplet state is surprisingly small, ~10(7) s(-1), prese

223 hat Dexter electron exchange from the ligand triplet state is the dominant energy transfer mechanism

224 interactions between the substrates, and the triplet state reaction paths.

225 erno-Buchi reaction that utilizes the unique triplet state reactivity of oximes, specifically 2-isoxa

226 t intersystem crossing to the lowest excited triplet state upon halogenation was a key mechanistic st

227 As compared to the singlet state, in the triplet state, the Gibbs barrier for the attack to the [

228 molytic cleavage of the RN-NO(2) bond in the triplet state.

229 higher vibrational level of the isoenergetic triplet state.

230 iltonian to describe the dynamics of the two-triplet state.

231 tes from a pair of excitations to the second triplet state.

232 limited by rapid intersystem crossing to the triplet state.

233 We show that the Baird aromatic triplet-state energy of cyclooctatetraene can be physica

234 To favor triplet-state formation as required for singlet oxygen g

235 UV photoproducts of tryptophan yield excited triplet-state organic matters during sunlight irradiatio

236 oupled cluster [DLPNO-CCSD(T)] theory reveal triplet-state wavefunction spatial distributions consist

237 gy separation between the lowest singlet and triplet states (Delta E(S(1)-T(1)) = 500 cm(-1)) and an

238 "Self-healing" dyes, in which triplet states are intramolecularly quenched, enable flu

239 rgies of charge transfer and locally excited triplet states influence the performance of the deep-blu

240 lexes, zeta-carotene does not quench excited triplet states of BChl a, likely due to elevation of the

241 eactive intermediates (RIs), such as excited triplet states of dissolved organic matter ((3)DOM*), si

242 es are vital for the effective population of triplet states.

243 t charge-transfer states and amide-localized triplet states.

244 d computational studies usually characterize triplet streaming either during alternations or during b

245 ations about the upcoming label based on the triplet structure and were surprised when it happened to

246 etic fluctuations are argued to lead to spin-triplet superconductivity from pairing between opposite

247 nsidered ideal candidates for realizing spin-triplet superconductivity(4).

248 Spin-triplet superconductors are condensates of electron pair

249 Triplet syn-2-formyl-3-fluorophenylnitrene, generated in

250 ses, the distinguishability of the molecular triplets-that is, the extent of orbital overlap-determin

251 (5) C loss leads to ribosome stalling at UUG triplets, the only codon translated by an m(5) C34-modif

252 ohort D) or 1.8 mg/kg (cohort E); and in the triplet therapy group fixed nivolumab 3 mg/kg and ipilim

253 in the nivolumab group, and 11 (50%) in the triplet therapy group including: eight (13%) of 64 patie

254 roup), nivolumab (nivolumab group), or both (triplet therapy group) using a 3 + 3 dose escalation des

255 the nivolumab group, and 82% (60-95) in the triplet therapy group, and the complete response rate wa

256 olumab group, and 1.7 years (1.6-1.9) in the triplet therapy group, median progression-free survival

257 e ipilimumab group and every 12 weeks in the triplet therapy group.

258 the nivolumab group, and 73% (50-89%) in the triplet therapy group.

259 s, one in the nivolumab group and one in the triplet therapy group.

260 , brentuximab vedotin with nivolumab and the triplet therapy, are being compared in a randomised phas

261 itation to be a transition from a Zhang-Rice triplet to a Zhang-Rice singlet.

262 the reverse intersystem crossing (RISC) from triplet to singlet exciplex diminishes, a pronounced iso

263 sm involving heavy-atom QMT through crossing triplet to singlet potential energy surfaces.

264 iplets to gain oscillator strength, enabling triplets to be directly generated on molecules via photo

265 om the ground-state singlet to excited-state triplets to gain oscillator strength, enabling triplets

266 to-photoluminescence studies reveal that the triplet-to-singlet conversion in exciplexes involves an

267 The results of our work indicate successful triplet-to-singlet energy transfer and a sizable increas

268 o Cy in their triplet excited state and then triplet-to-singlet intersystem crossing in the nascent g

269 e molecular motor pillars confirms efficient triplet-to-triplet energy transfer between the porphyrin

270 that UTe(2) is a strong candidate for chiral-triplet topological superconductivity.

271 y unfavourable and spectroscopy shows direct triplet transfer from nanocrystals to naphthalene; nonet

272 tracene is energetically favoured, and hence triplet transfer proceeds via a charge separated state.

273 e range [Formula: see text] = 3-9 D with the triplet transitions consistently showing shorter charge

274 latory activity in the beta band (~20 Hz) at triplet transitions that indexes learning: it emerges wi

275 ized that hypophosphorylation of Cx43 serine-triplet triggers pathological Cx43 redistribution to the

276 Sensitized triplet-triplet annihilation (sTTA) is the most promisin

277 Photon upconversion via triplet-triplet annihilation (TTA) has achieved high eff

278 iplet excited states, enhancing the yield of triplet-triplet annihilation and promoting radiative dec

279 an intermediate in both singlet fission and triplet-triplet annihilation and that this is true for b

280 ile delayed fluorescence results mainly from triplet-triplet annihilation at lower temperatures in TH

281 Triplet-triplet annihilation based molecular photon upco

282 At lower temperatures triplet-triplet annihilation dominates.

283 stinct (1)(TT) emission arises directly from triplet-triplet annihilation in high-quality pentacene s

284 o triplet excitons, the limiting step is the triplet-triplet annihilation pathway, where the kinetics

285 Singlet fission and triplet-triplet annihilation represent two highly promis

286 Triplet-triplet annihilation upconversion (TTA-UC) is an

287 has been debate over the role of (1)(TT) in triplet-triplet annihilation.

288 to the substrate or to a co-catalyst through triplet-triplet energy transfer (TT EnT).

289 + 2] cycloaddition, which is initiated by a triplet-triplet energy transfer process.

290 Specifically, we compare the triplet-triplet exchange (J) for tetracene dimers, bipen

291 f excited-state lifetime extension utilizing triplet-triplet excited-state equilibria is detailed.

292 tensities, reflecting thermal activation and triplet-triplet exciton annihilation processes.

293 dressable defect sites, we designed the spin-triplet, V(3+) complex, (C(6)F(5))(3)trenVCN(t)Bu (1).

294 ges associate with two centriole microtubule triplets via an elaborate filamentous base and that they

295 ed knockin mdx mice in which the Cx43 serine-triplet was replaced with either phospho-mimicking gluta

296 orbit coupling (SOC) between the singlet and triplet wavefunctions.

297 X-ray diffraction as a solvent-separated ion triplet with two potassium counterions.

298 nd the frequency and position of the altered triplets within long stretches of d(CGA) triplets.

299 order caused by an abnormal expansion of GCN triplets within the PABPN1 gene.

300 t pair separation, giving rise to an overall triplet yield of 181 %.