The 2.2 A crystal structure of a pocilloporin pigment reveals a nonplanar chromophore conformation

Reef-building corals contain host pigments, termed pocilloporins, that function to regulate the light environment of their resident microalgae by acting as a photoprotectant in excessive sunlight. We have determined the crystal structure of an intensely blue, nonfluorescent pocilloporin to 2.2 A resolution and a genetically engineered fluorescent variant to 2.4 A resolution. The pocilloporin chromophore structure adopts a markedly different conformation in comparison with the DsRed chromophore, despite the chromophore sequences (Gln-Tyr-Gly) being identical; the tyrosine ring of the pocilloporin chromophore is noncoplanar and in the trans configuration. Furthermore, the fluorescent variant adopted a noncoplanar chromophore conformation. The data presented here demonstrates that the conformation of the chromophore is highly dependent on its immediate environment.     

The retinal conformation and its environment in rhodopsin in light of a new 2.2 A crystal structure

A new high-resolution structure is reported for bovine rhodopsin, the visual pigment in rod photoreceptor cells. Substantial improvement of the resolution limit to 2.2 A has been achieved by new crystallization conditions, which also reduce significantly the probability of merohedral twinning in the crystals. The new structure completely resolves the polypeptide chain and provides further details of the chromophore binding site including the configuration about the C6-C7 single bond of the 11-cis-retinal Schiff base. Based on both an earlier structure and the new improved model of the protein, a theoretical study of the chromophore geometry has been carried out using combined quantum mechanics/force field molecular dynamics. The consistency between the experimental and calculated chromophore structures is found to be significantly improved for the 2.2 A model, including the angle of the negatively twisted 6-s-cis-bond. Importantly, the new crystal structure refinement reveals significant negative pre-twist of the C11-C12 double bond and this is also supported by the theoretical calculation although the latter converges to a smaller value. Bond alternation along the unsaturated chain is significant, but weaker in the calculated structure than the one obtained from the X-ray data. Other differences between the experimental and theoretical structures in the chromophore binding site are discussed with respect to the unique spectral properties and excited state reactivity of the chromophore.     

Solution structures of C-1027 apoprotein and its complex with the aromatized chromophore

C-1027 is one of the most potent antitumor antibiotic chromoproteins, and is a 1:1 complex of an enediyne chromophore having DNA-cleaving ability and a carrier apoprotein. The three-dimensional solution structures of the 110 residue (10.5 kDa) C-1027 apoprotein and its complex with the aromatized chromophore have been determined separately by homonuclear two-dimensional nuclear magnetic resonance methods. The apoprotein is mainly composed of three antiparallel beta-sheets: four-stranded beta-sheet (43-45, 52-54; 30-38; 92-94; 104-106), three-stranded beta-sheet (4-6; 17-22; 61-66), and two-stranded beta-sheet (70-72; 83-85). The overall structure of the apoprotein is very similar to those of other chromoprotein apoproteins, such as neocarzinostatin and kedarcidin. A hydrophobic pocket with approximate dimensions of 14 A x 12 A x 8 A is formed by the four-stranded beta-sheet and the three loops (39-42; 75-79; 97-100). The holoprotein (complex form with the aromatized chromophore) structure reveals that the aromatized chromophore is bound to the hydrophobic pocket found in the apoprotein. The benzodihydropentalene core of the chromophore is located in the center of the pocket and other substituents (beta-tyrosine, benzoxazine, and aminosugar moieties) are arranged around the core. Major binding interactions between the apoprotein and the chromophore are likely the hydrophobic contacts between the core of the chromophore and the hydrophobic side-chains of the pocket-forming residues, which is supplemented by salt bridges and/or hydrogen bonds. Based on the holoprotein structure, we propose possible mechanisms for the stabilization and the release of chromophore by the apoprotein.     

The microenvironment around the chromophores and its changes due to the association states in C-phycocyanin isolated from the cyanobacterium Mastigocladus laminosus

The chromophore-protein interaction in C-phycocyanin was investigated as a function of the association state of the protein. Changes in the microenvironment around the chromophores were monitored by the following three indices: (1) the accessibility of a small molecule to the chromophore; (2) the fluorescence from aromatic amino acid residues; and (3) the effect of configurational changes of the chromophore on the conformation of the polypeptide chain. In the C-phycocyanin trimer, all the chromophores are shielded from the aqueous phase, probably by contact between subunits, and by a loop structure which surrounds the chromophores, even though that loop structure is not shown by X-ray analysis (Schirmer, T., Bode, W., Huber, R., Sidler, W. and Zuber, H. (1985) J. Mol. Biol. 184, 257–277). The polypeptide folding depends on the electronic structure of the chromophores; the oxidized chromophore of the α subunit inhibits the formation of the trimer and the reduced state of the chromophore of the α subunit allows the formation of trimers, in which the chromophores have the same electronic structure as in the monomers. The fluorescence from the aromatic amino acid residues showed that the conformational changes were induced by the reduced chromophore. These results indicate that the chromophore structure and the protein conformation affect each other. A definite configuration of the chromophore and also a definite conformation of the polypeptide are necessary for the intact energy transfer within C-phycocyanin.     

The 2.1A crystal structure of copGFP, a representative member of the copepod clade within the green fluorescent protein superfamily

The green fluorescent protein (avGFP), its variants, and the closely related GFP-like proteins are characterized structurally by a cyclic tri-peptide chromophore located centrally within a conserved beta-can fold. Traditionally, these GFP family members have been isolated from the Cnidaria although recently, distantly related GFP-like proteins from the Bilateria, a sister group of the Cnidaria have been described, although no representative structure from this phylum has been reported to date. We have determined to 2.1A resolution the crystal structure of copGFP, a representative GFP-like protein from a copepod, a member of the Bilateria. The structure of copGFP revealed that, despite sharing only 19% sequence identity with GFP, the tri-peptide chromophore (Gly57-Tyr58-Gly59) of copGFP adopted a cis coplanar conformation within the conserved beta-can fold. However, the immediate environment surrounding the chromophore of copGFP was markedly atypical when compared to other members of the GFP-superfamily, with a large network of bulky residues observed to surround the chromophore. Arg87 and Glu222 (GFP numbering 96 and 222), the only two residues conserved between copGFP, GFP and GFP-like proteins are involved in autocatalytic genesis of the chromophore. Accordingly, the copGFP structure provides an alternative platform for the development of a new suite of fluorescent protein tools. Moreover, the structure suggests that the autocatalytic genesis of the chromophore is remarkably tolerant to a high degree of sequence and structural variation within the beta-can fold of the GFP superfamily.     

Synthesis and properties of the chromophore of the asFP595 chromoprotein from Anemonia sulcata

A model compound for the chromophore within the purple nonfluorescent GFP-like chromoprotein asFP595 was synthesized. The postulated structure of the chromophore, 2-acetyl-4-(p-hydroxybenzylidene)-1-methyl-5-imidazolone, was taken from the high-resolution crystal structure analysis of intact asFP595 [Quillin, M. L., Anstrom, D., Shu, X., O'Leary, S., Kallio, K., Lukyanov, K. A., and Remington, S. J. (2005) Kindling Fluorescent Protein from Anemonia sulcata: Dark-State Structure at 1.38 A Resolution, Biochemistry 44, 5774-5787]. Erlenmeyer lactonization and oxidation of the methylene group attached to the heteroaromatic moiety with selenium dioxide were used at the key stages of the synthesis. The spectral properties of the model chromophore in solution and their dependence on the pH and polarity of the solvent were investigated. In water, the chromophore was found to exist in two forms, neutral and anionic, with a pK(a) of 7.1. In a dimethylformamide solution, the spectral properties of the anionic form closely match those of the native protein, demonstrating that under these conditions, the compound is an excellent model for the chromophore within native asFP595.     

Crystallographic structures of Discosoma red fluorescent protein with immature and mature chromophores: linking peptide bond trans-cis isomerization and acylimine formation in chromophore maturation

The mature self-synthesizing p-hydroxybenzylideneimidazolinone-like fluorophores of Discosoma red fluorescent protein (DsRed) and Aequorea victoria green fluorescent protein (GFP) are extensively studied as powerful biological markers. Yet, the spontaneous formation of these fluorophores by cyclization, oxidation, and dehydration reactions of tripeptides within their protein environment remains incompletely understood. The mature DsRed fluorophore (Gln 66, Tyr 67, and Gly 68) differs from the GFP fluorophore by an acylimine that results in Gln 66 Calpha planar geometry and by a Phe 65-Gln 66 cis peptide bond. DsRed green-to-red maturation includes a green-fluorescing immature chromophore and requires a chromophore peptide bond trans-cis isomerization that is slow and incomplete. To clarify the unique structural chemistry for the individual immature "green" and mature "red" chromophores of DsRed, we report here the determination and analysis of crystal structures for the wild-type protein (1.4 A resolution), the entirely green DsRed K70M mutant protein (1.9 A resolution), and the DsRed designed mutant Q66M (1.9 A resolution), which shows increased red chromophore relative to the wild-type DsRed. Whereas the mature, red-fluorescing chromophore has the expected cis peptide bond and a sp(2)-hybridized Gln 66 Calpha with planar geometry, the crystal structure of the immature green-fluorescing chromophore of DsRed, presented here for the first time, reveals a trans peptide bond and a sp(3)-hybridized Gln 66 Calpha with tetrahedral geometry. These results characterize a GFP-like immature green DsRed chromophore structure, reveal distinct mature and immature chromophore environments, and furthermore provide evidence for the coupling of acylimine formation with trans-cis isomerization.     

Probing the ground state structure of the green fluorescent protein chromophore using Raman spectroscopy

We present Raman spectra, obtained using 752 nm excitation, on wild-type GFP and the S65T mutant of this intrinsically fluorescent protein together with data on a model chromophore, ethyl 4-(4-hydroxyphenyl)methylidene-2-methyl-5-oxoimidazolacetate . In the pH range 1-14, the model compound has two macroscopic pK(a)s of 1.8 and 8.2 attributed to ionization of the imidazolinone ring nitrogen and the phenolic hydroxyl group, respectively. Comparison of the model chromophore with the chromophore in wild-type GFP and the S65T mutant reveals that the cationic form, with both the imidazolinone ring nitrogen and the phenolic oxygen protonated, is not present in these particular GFP proteins. Our results do not provide any evidence for the zwitterionic form of the chromophore, with the phenolic group deprotonated and the imidazolinone ring nitrogen protonated, being present in the GFP proteins. In addition, since the position of the Raman bands is a property exclusively of the ground state structure, the data enable us to investigate how protein-chromophore interactions affect the ground state structure of the chromophore without contributions from excited state effects. It is found that the ground state structure of the anionic form of the chromophore, which is most relevant to the fluorescent properties, is strongly dependent on the chromophore environment whereas the neutral form seems to be insensitive. A linear correlation between the absorption properties and the ground state structure is demonstrated by plotting the absorption maxima versus the wavenumber of a Raman band found in the range 1610-1655 cm(-1).     

Dynamics of protein and chromophore structural changes in the photocycle of photoactive yellow protein monitored by time-resolved optical rotatory dispersion

The dynamics of the PYP photocycle have been studied using time-resolved optical rotatory dispersion (TRORD) spectroscopy in the visible and far-UV spectral regions to probe the changes in the chromophore configuration and the protein secondary structure, respectively. The changes in the secondary structure in PYP upon photoisomerization of the chromophore can be described by two exponential lifetimes of 2 +/- 0.8 and 650 +/- 100 ms that correspond to unfolding and refolding processes, respectively. The TRORD experiments that follow the dynamics of the chromophore report three exponential components, with lifetimes of 10 +/- 3 micros, 1.5 +/- 0.5 ms, and 515 +/- 110 ms. A comparison of the kinetic behaviors of the chromophore and protein shows that during the decay of pR(465) an initial relaxation that is localized to the chromophore hydrophobic pocket precedes the formation of the chromophore and protein structures found in pB(355). In contrast, the protein and chromophore processes occur with similar time constants during inactivation of the signaling state.     

The 2.1A crystal structure of the far-red fluorescent protein HcRed: inherent conformational flexibility of the chromophore

We have determined the crystal structure of HcRed, a far-red fluorescent protein isolated from Heteractis crispa, to 2.1A resolution. HcRed was observed to form a dimer, in contrast to the monomeric form of green fluorescent protein (GFP) or the tetrameric forms of the GFP-like proteins (eqFP611, Rtms5 and DsRed). Unlike the well-defined chromophore conformation observed in GFP and the GFP-like proteins, the HcRed chromophore was observed to be considerably mobile. Within the HcRed structure, the cyclic tripeptide chromophore, Glu(64)-Tyr(65)-Gly(66), was observed to adopt both a cis coplanar and a trans non-coplanar conformation. As a result of these two conformations, the hydroxyphenyl moiety of the chromophore makes distinct interactions within the interior of the beta-can. These data together with a quantum chemical model of the chromophore, suggest the cis coplanar conformation to be consistent with the fluorescent properties of HcRed, and the trans non-coplanar conformation to be consistent with non-fluorescent properties of hcCP, the chromoprotein parent of HcRed. Moreover, within the GFP-like family, it appears that where conformational freedom is permissible then flexibility in the chromophore conformation is possible.     

Chromophore-protein interactions in the anthozoan green fluorescent protein asFP499

Despite their similar fold topologies, anthozoan fluorescent proteins (FPs) can exhibit widely different optical properties, arising either from chemical modification of the chromophore itself or from specific interactions of the chromophore with the surrounding protein moiety. Here we present a structural and spectroscopic investigation of the green FP asFP499 from the sea anemone Anemonia sulcata var. rufescens to explore the effects of the protein environment on the chromophore. The optical absorption and fluorescence spectra reveal two discrete species populated in significant proportions over a wide pH range. Moreover, multiple protonation reactions are evident from the observed pH-dependent spectral changes. The x-ray structure of asFP499, determined by molecular replacement at a resolution of 1.85 A, shows the typical beta-barrel fold of the green FP from Aequorea victoria (avGFP). In its center, the chromophore, formed from the tripeptide Gln(63)-Tyr(64)-Gly(65), is tightly held by multiple hydrogen bonds in a polar cage that is structurally quite dissimilar to that of avGFP. The x-ray structure provides interesting clues as to how the spectroscopic properties are fine tuned by the chromophore environment.     

Chromophore equilibria in bacteriorhodopsin.

An investigation of the dark equilibria between different chromophores of bacteriorhodopsin (BR) and studies of the kinetics of their interconversion and photochemical activity have led to the following conclusions. (a) A component of the 605-nm chromophore of BR decays in the millisecond range and is likely to be identical to the intermediate O of the photochemical cycle of BR and is assumed to be formed from the purple complex (PC) by the binding of one proton to BR. (b) An acidic form the PC, PCaL-, arises from the 605-nm chromophore by selective binding of anions L- (F- greater than Cl- greater than Br- greater than I- greater than Cl04-) to BR. (c) The isomeric equilibrium between 13-cis and all-trans retinal is approximately 0.15/0.85 in PCaCl-, 0.3/0.7 in the 605-nm chromophore as compared to 0.5/0.5 in the PC. (d) The 500-nm chromophore is formed from the PC by release of nearly one proton from BR. (e) The pH range in which the PC exists is reduced in a high-temperature structure of the purple membrane as compared to its low temperature structure. A model for the chromophore structure is proposed as a hypothesis, which allows a comprehensive interpretation of the results. In this model the absorption spectrum of the retinylidene lysine Schiff base is modulated by its protonation state and the interaction with an anionic group.     

Structural characterization of a thiazoline-containing chromophore in an orange fluorescent protein, monomeric Kusabira Orange

Monomeric Kusabira Orange (mKO) is a green fluorescent protein (GFP)-like protein that emits orange light at a peak of 559 nm. We analyzed its X-ray structure at 1.65 A and found a novel three-ring chromophore that developed autocatalytically from a Cys65-Tyr66-Glu67 tripeptide in which the side chain of Cys65 formed the third 2-hydroxy-3-thiazoline ring. As a result, the chromophore contained the CNCOH group at the 2-position of the imidazolinone moiety such that the conjugated pi-electron system of the chromophore was more extended than that of GFP but less extended than that of the Discosoma sp. red fluorescent protein (DsRed). Since a sulfur atom has potent nucleophilic character, the third 3-thiazoline ring is rapidly and completely cyclized. Furthermore, our structure reveals the presence of a pi-pi stacking interaction between His197 and the chromophore as well as a pi-cation interaction between Arg69 and the chromophore. These structural findings are sufficient to account for the orange emission, pH tolerance, and photostability of mKO.     

Molecular mechanism of spectral tuning in sensory rhodopsin II.

Sensory rhodopsin II (SRII) is unique among the archaeal rhodopsins in having an absorption maximum near 500 nm, blue shifted roughly 70 nm from the other pigments. In addition, SRII displays vibronic structure in the lambda(max) absorption band, whereas the other pigments display fully broadened band maxima. The molecular origins responsible for both photophysical properties are examined here with reference to the 2.4 A crystal structure of sensory rhodopsin II (NpSRII) from Natronobacterium pharaonis. We use semiempirical molecular orbital theory (MOZYME) to optimize the chromophore within the chromophore binding site, and MNDO-PSDCI molecular orbital theory to calculate the spectroscopic properties. The entire first shell of the chromophore binding site is included in the MNDO-PSDCI SCF calculation, and full single and double configuration interaction is included for the chromophore pi-system. Through a comparison of corresponding calculations on the 1.55 A crystal structure of bacteriorhodopsin (bR), we identify the principal molecular mechanisms, and residues, responsible for the spectral blue shift in NpSRII. We conclude that the major source of the blue shift is associated with the significantly different positions of Arg-72 (Arg-82 in bR) in the two proteins. In NpSRII, this side chain has moved away from the chromophore Schiff base nitrogen and closer to the beta-ionylidene ring. This shift in position transfers this positively charged residue from a region of chromophore destabilization in bR to a region of chromophore stabilization in NpSRII, and is responsible for roughly half of the blue shift. Other important contributors include Asp-201, Thr-204, Tyr-174, Trp-76, and W402, the water molecule hydrogen bonded to the Schiff base proton. The W402 contribution, however, is a secondary effect that can be traced to the transposition of Arg-72. Indeed, secondary interactions among the residues contribute significantly to the properties of the binding site. We attribute the increased vibronic structure in NpSRII to the loss of Arg-72 dynamic inhomogeneity, and an increase in the intensity of the second excited (1)A(g)(-) -like state, which now appears as a separate feature within the lambda(max) band profile. The strongly allowed (1)B(u)(+)-like state and the higher-energy (1)A(g)(-) -like state are highly mixed in NpSRII, and the latter state borrows intensity from the former to achieve an observable oscillator strength.     

Variations on the GFP chromophore: A polypeptide fragmentation within the chromophore revealed in the 2.1-A crystal structure of a nonfluorescent chromoprotein from Anemonia sulcata

We have determined to 2.1 A resolution the crystal structure of a dark state, kindling fluorescent protein isolated from the sea anemone, Anemonia sulcata. The chromophore sequence Met(63)-Tyr(64)-Gly(65) of the A. sulcata chromoprotein was previously proposed to comprise a 6-membered pyrazine-type heterocycle (Martynov, V. I., Savitsky, A. P., Martynova, N. Y., Savitsky, P. A., Lukyanov, K. A., and Lukyanov, S. A. (2001) J. Biol. Chem. 276, 21012-21016). However, our crystallographic data revealed the chromophore to comprise a 5-membered p-hydroxybenzylideneimidazolinone moiety that adopts a non-coplanar trans conformation within the interior of the GFP beta-can fold. Unexpectedly, fragmentation of the polypeptide was found to occur within the chromophore moiety, at the bond between Cys(62C) and Met(63N1.) Our structural data reveal that fragmentation of the chromophore represents an intrinsic, autocatalytic step toward the formation of the mature chromophore within the specific GFP-like proteins.     

The 2.0-A crystal structure of eqFP611, a far red fluorescent protein from the sea anemone Entacmaea quadricolor

We have crystallized and subsequently determined to 2.0-A resolution the crystal structure of eqFP611, a far red fluorescent protein from the sea anemone Entacmaea quadricolor. The structure of the protomer, which adopts a beta-can topology, is similar to that of the related monomeric green fluorescent protein (GFP). The quaternary structure of eqFP611, a tetramer exhibiting 222 symmetry, is similar to that observed for the more closely related red fluorescent protein DsRed and the chromoprotein Rtms5. The unique chromophore sequence (Met63-Tyr64-Gly65) of eqFP611, adopts a coplanar and trans conformation within the interior of the beta-can fold. Accordingly, the eqFP611 chromophore adopts a significantly different conformation in comparison to the chromophore conformation observed in GFP, DsRed, and Rtms5. The coplanar chromophore conformation and its immediate environment provide a structural basis for the far red, highly fluorescent nature of eqFP611. The eqFP611 structure extends our knowledge on the range of conformations a chromophore can adopt within closely related members of the green fluorescent protein family.     

A structural basis for the pH-dependent increase in fluorescence efficiency of chromoproteins

Within the fluorescent protein and chromoprotein family, the phenomenon of photoswitching is both intriguing and biotechnologically useful. Illumination of particular chromoproteins with intense light results in dramatic increases in fluorescence efficiency (termed kindling) and involves cis-trans isomerization of the chromophore. Here we report that chromophore isomerization can also be driven via alteration in pH. Specifically, we demonstrate that a number of naturally occurring chromoproteins, and their engineered variants, undergo a dramatic 20-100-fold increase in fluorescence efficiency at alkaline pH (>pH9.0). We have determined to 1.8 A resolution the structure of one such chromoprotein, Rtms5(H146S), in its highly far-red fluorescent form (Phi(F), 0.11 at pH 10.7) and compared it to the structure of the non-fluorescent form (Phi(F), 0.002 at pH 8.0). At high pH, the cyclic tri-peptide chromophore was observed to be mobile and distributed between a trans non-coplanar and a cis coplanar conformation, whereas at the lower pH, only a trans non-coplanar chromophore was observed. Calculation of pK(a) values suggested that titration of the side-chain of the conserved Glu215 close to the chromophore is involved in promoting the cis-coplanar conformation. Collectively, our data establish that isomerization to form a coplanar chromophore is a basis of the increased fluorescence efficiency at high pH. The phenomenon of pH-induced fluorescence gain has similarities with photoswitching, thereby providing a model to study the mechanism of kindling.     

Dependence of Mode of DNA Binding to Benzocrown Derivatives of Actinocin on the Size and Distance from the Chromophore of Crown Fragments

Complexes of DNA with benzocrown derivatives of actinocin were studied by viscometry and dynamic birefringence. Changes in the macromolecular structure of DNA caused by complex formation were determined. Models of DNA binding to the studied compounds were suggested on the basis of data obtained. The intercalation of actinocin chromophore of benzocrown derivatives of actinocin was shown to occur only when benzocrown groups were bound to the chromophore via the glycine spacer. A change of the distance between the crown group and the chromophore prevented ligand intercalation. Increase of the ionic strength resulted in appearance of a new, nonintercalative binding mode for crown-containing compounds determined by interaction of the crown groups with DNA.     

Solid-state NMR spectroscopic study of chromophore-protein interactions in the Pr ground state of plant phytochrome A

Despite extensive study, the molecular structure of the chromophore-binding pocket of phytochrome A (phyA), the principal photoreceptor controlling photomorphogenesis in plants, has not yet been successfully resolved. Here, we report a series of two-dimensional (2-D) magic-angle spinning solid-state NMR experiments on the recombinant N-terminal, 65-kDa PAS-GAF-PHY light-sensing module of phytochrome A3 from oat (Avena sativa), assembled with uniformly 13C- and 15N-labeled phycocyanobilin (u-[13C,15N]-PCB-As.phyA3). The Pr state of this protein was studied regarding the electronic structure of the chromophore and its interactions with the proximal amino acids. Using 2-D 13C-13C and 1H-15N experiments, a complete set of 13C and 15N assignments for the chromophore were obtained. Also, a large number of 1H-13C distance restraints between the chromophore and its binding pocket were revealed by interfacial heteronuclear correlation spectroscopy. 13C doublings of the chromophore A-ring region and the C-ring carboxylate moiety, together with the observation of two Pr isoforms, Pr-I and Pr-II, demonstrate the local mobility of the chromophore and the plasticity of its protein environment. It appears that the interactions and dynamics in the binding pocket of phyA in the Pr state are remarkably similar to those of cyanobacterial phytochrome (Cph1). The N-terminus of the region modeled (residues 56-66 of phyA) is highly mobile. Differences in the regulatory processes involved in plant and Cph1 phytochromes are discussed.     

Probing the structural determinants of yellow fluorescence of a protein from Phialidium sp

Fluorescent proteins homologous to green fluorescent protein (avGFP) display pronounced spectral variability due to different chromophore structures and variable chromophore interactions with the surrounding amino acids. To gain insight into the structural basis for yellow emission, the 3D structure of phiYFP (λ_em = 537 nm), a protein from the sea medusa Phialidium sp., was built by a combined homology modeling – mass spectrometry approach. Mass spectrometry of the isolated chromophore-bearing peptide reveals that the chromophore of phiYFP is chemically identical to that of avGFP (λ_em = 508 nm). The experimentally acquired chromophore structure was combined with the homology-based model of phiYFP, and the proposed 3D structure was used as a starting point for identification of the structural features responsible for yellow fluorescence. Mutagenesis of residues in the local chromophore environment of phiYFP suggests that multiple factors cooperate to establish the longest-wavelength emission maximum among fluorescent proteins with an unmodified GFP-like chromophore.