Abstract
Alteration in mitochondrial transmembrane potential (ΔΨm) is an important characteristic of cancer. The observation that the enhanced negative mitochondrial potential is prevalent in tumor cell phenotype provides a conceptual basis for development of mitochondrion-targeting therapeutic drugs and molecular imaging probes. Since plasma and mitochondrial potentials are negative, many delocalized organic cations, such as rhodamine-123 and 3H-tetraphenylphosphonium, are electrophoretically driven through these membranes, and able to localize in the energized mitochondria of tumor cells. Cationic radiotracers, such as 99mTc-Sestamibi and 99mTc-Tetrofosmin, have been clinically used for diagnosis of cancer by single photon emission computed tomography (SPECT) and noninvasive monitoring of the multidrug resistance (MDR) transport function in tumors of different origin. However, their diagnostic and prognostic values are often limited due to their insufficient tumor localization (low radiotracer tumor uptake) and high radioactivity accumulation in the chest and abdominal regions (low tumor selectivity). In contrast, the 64Cu-labeled phosphonium cations represent a new class of PET (positron emission tomography) radiotracers with good tumor uptake and high tumor selectivity. This review article will focus on our recent experiences in evaluation of 64Cu-labeled phosphonium cations as potential PET radiotracers. The main objective is to illustrate the impact of radiometal chelate on physical, chemical and biological properties of 64Cu radiotracers. It will also discuss some important issues related to their tumor selectivity and possible tumor localization mechanism.
Keywords: 64Cu, phosphonium cations, tumor imaging and PET
Introduction
Early Detection of Cancer
Cancer is the second leading cause of death worldwide. The most prevalent forms of this disease are solid tumors of the lung, breast, prostate, colon and rectum.1 Most cancer patients can survive for a long period of time after surgery, radiation and chemotherapy or a combination thereof if it can be detected at the early stage. Therefore, accurate early detection is highly desirable so that various therapeutic regimens can be given before tumors become widely spread. Many imaging modalities are currently available for early cancer detection. Ultrasonography (US), computed tomography (CT) and magnetic resonance imaging (MRI) can provide details of structural changes, variations in density and differences in proton content in tissues. However, it remains a significant challenge to use US, CT and MRI methods for molecular imaging of cancer. Nuclear medicine procedures using radiolabeled receptor ligands can provide the in vivo characterization of cellular structure, and are able to monitor biological changes in tumor tissues at the cellular and molecular levels. A “fatal flaw” for most of the receptor-based target-specific radiotracers is that not all tumors over-express that specific receptor. Thus, it is of great benefit to develop a molecular imaging probe that could detect cancers by targeting a biomarker found in majority, if not all, of human cancer lesions.
Targeting Energized Mitochondria
Alteration in mitochondrial transmembrane potential (Δ Ψm) is an important characteristic of cancer caused directly by mitochondrial dysfunction, such as DNA mutation and oxidative stress.2–5 It has been reported that the mitochondrial transmembrane potential in carcinoma cells (regardless of the tumor origin) is significantly higher than that in normal epithelial cells.6–11 For example, the difference in ΔΨm between the colon carcinoma cell line CX-1 and the control green monkey kidney epithelial cell line CV-1 was approximately 60 mV (163 mV in tumor cells vs. 104 mV in normal cells). The observation that the enhanced negative mitochondrial potential is prevalent in tumor cell phenotype provides the conceptual basis for development of mitochondrion-targeting therapeutic pharmaceuticals and molecular imaging probes.2–5, 12–25
Measuring Mitochondrial Potential with Lipophilic Organic Cations
Mitochondrial potential measurement provides the most comprehensive reflection of mitochondrial bio-energetic function primarily because it directly depends on the proper integration of diverse metabolic pathways that converge at mitochondria. Since both plasma and mitochondrial potentials are negative, many delocalized cationic molecules with appropriate structural features are electrophoretically driven through these transmembranes, and tend to accumulate inside the energized mitochondria of tumor cells.2–5, 12–17 This is exemplified by the use of rhodamine-123 and 3H-tetraphenylphosphonium (3H-TPP) for measurement of mitochondrial potential in tumor cells on the basis of their intracellular and mitochondrial concentration.6–10, 13, 15, 16 In addition, rhodamine derivatives have also been used as fluorescent probes for optical imaging of tumors n animal models.18–25
Imaging Tumors with Cationic Radiotracers
Cationic radiotracers, such as 99mTc-Sestamibi and 99mTc-Tetrofosmin, were developed as radiotracers for myocardial perfusion imaging by single photon emission computed tomography (SPECT).26–31 It was found that these cationic radiotracers are also able to localize in tumors due to the increased negative plasma and mitochondrial potential in tumor cells as compared to normal cells of surrounding tissues.32–42 99mTc-Sestamibi and 99mTc-Tetrofosmin have been clinically used for diagnosis of cancer and noninvasive monitoring of the tumor multidrug resistance (MDR) transport function.33, 36–42 However, their diagnostic and prognostic values are often limited due to their insufficient tumor localization and high radioactivity accumulation in the chest and abdominal regions.
Radiolabeled Phosphonium Cations as Radiotracers
More than 20 years ago, radiolabeled quaternary ammonium, phosphonium and arsonium cations were studied as perfusion radiotracers for heart imaging.43, 44 Recently, several groups proposed to use radiolabeled triphenylphosphonium, such as 4-(18F-benzyl)triphenylphosphonium (18F-BzTPP), cations as PET radiotracers for myocardial perfusion and tumor imaging.45–52 It has been reported that 3H-tetraphenylphosphonium (3H-TPP) has better tumor uptake than 99mTc-Sestamibi;53 but its tumor selectivity is poor with tumor/heart ratios «1.0. Since 3H-TPP is not suitable for PET imaging, the 11C-labeled TPP cation has been proposed as the alternative.45, 46 In addition, the high uptake of 18F-BzTPP in the heart and liver may impose a significant challenge for its application in diagnosis of cancer in chest and abdominal regions. Even though biodistribution and imaging studies in small animals45, 52 and dogs45, 46, 49 have clearly demonstrated the utility of 11C and 18F-labeled TPP cations for imaging heart and tumors by PET, the combination of short half-life of 11C (T1/2 = 20.4 min, 98% abundance) and 18F (T1/2 = 110 min, 97% abundance) with their poor availability and high cost of infrastructure makes it very difficult to use 11C and 18F-labeled TPP cations for PET studies of cancer patients in most of the clinic settings. Therefore, there is an urgent need for new and better PET radiotracers that can be readily prepared, have high tumor-selectivity, and are able to provide the information of the tumor mitochondrial function in a noninvasive fashion.
About This Review
Many review articles appeared covering the nuclear medicine applications of cationic radiotracers for tumor imaging and noninvasive monitoring of tumor MDR transport function by SPECT or PET.36–42 This article is not intended to be an exhaustive review of current literature on cationic radiotracers and their nuclear medicine applications. Instead, it will focus on our recent experiences in evaluations of 64Cu-labeled phosphonium cations as highly tumor-selective PET radiotracers. This review will also discuss some important issues related to their tumor selectivity and localization mechanism. The main objective is to illustrate the impact of bifunctional chelators (BFCs) and radiometal chelate on physical, chemical and biological properties of 64Cu-labeled phosphonium cations. It is very important to note that the mitochondrion-targeted radiotracers described in this article are not intended to measure the exact mitochondrial potential in tumor cells as 3H-TPP and the rhodamine derivatives are used for many in vitro assays.6–10, 13, 15, 16 Considering the heterogeneity of tumor cells in different regions of the same tumor tissue and among different types of tumors, these mitochondrion-targeted radiotracers are designed to noninvasively determine the contrast between the tumor and surrounding normal tissues.
Radiotracer Design and Synthesis
Characteristics of Optimal Radiotracers
For a new tumor-specific radiotracer to be successful, it must show clinical indications for high-incidence tumors (breast, lung and prostate cancers). The radiotracer should have high tumor uptake and target-to-background (T/B) ratios in a short period of time postinjection (p.i.). To achieve this goal, the radiotracer should have a rapid blood clearance to minimize background radioactivity. Since most high-incidence tumors occur in the chest and abdominal regions, renal excretion is needed to avoid excessive radioactivity accumulation in the gastrointestinal tract, which might interfere with interpretation of tumor radioactivity.
Radiotracer Design
Figure 1 shows selected phosphonium cations, bifunctional chelators (BFCs) and PKM (pharmacokinetic modifying) linkers. The phosphonium cation serves as a targeting moiety to carry 64Cu into the energized mitochondria of tumor cells. The BFC is required for chelation of 64Cu. PKM linkers are used to improve pharmacokinetics of 64Cu radiotracers. In principle, the 64Cu-labeled phosphonium cations should be useful for imaging most tumors, if not all, since the higher negative mitochondrial potential is prevalent in tumor cell phenotypes.47–53 Their high tumor selectivity provides a unique opportunity to develop radiotracers that are sensitive to the early change in tumor mitochondrial potential. Successful development of such a radiotracer will be beneficial for the early detection of cancer. It must be noted that the 64Cu-labeled phosphonium cations are significantly different from their 18F-analogs with respect to their physical, chemical and biological properties. Replacing 18F with a 64Cu-BFC chelate has significant impact on the biological characteristics of phosphonium cations due to its large size, hydrophilicity and the change in overall molecular charge.
Why 64Cu or 62Cu?
64Cu has a half-life of 12.7 h and a β+ emission (18%, Emax = 0.655 MeV). Despite its low β+ abundance, the long half-life makes it feasible to prepare, transport and deliver the 64Cu radiotracer for its clinical applications.54, 55 Recent breakthroughs in production of 64Cu with high specific activity have made it more available to small institutions without the on-site cyclotron facilities.54 Thus, 64Cu is a viable alternative to 18F for research programs that wish to incorporate high sensitivity and high spatial resolution of PET, but cannot afford to maintain the expensive radionuclide production infrastructure. 62Cu is a generator-produced radionuclide. Its 9.7 min half-life allows the repeated dosing without imposing a significant radiation burden to the patient. Copper radionuclides, related radiochemistry and nuclear medicine applications of 64Cu-radiotracers have been reviewed extensively.54–60 We have evaluated several metallic radionuclides (99mTc, 64Cu and 111In) for radiolabeling of phosphonium cations. It was found that only the 64Cu-labeled phosphonium cations are able to localize in U87MG glioma tumors with long tumor retention while the corresponding 99mTc and 111In radiotracers tend to have significant tumor washout. Since 64Cu and 62Cu share identical coordination chemistry, 62Cu-labeled phosphonium cations are expected to have the same biodistribution characteristics as their 64Cu analogs.
Bifunctional Chelators for 64Cu Chelation
Due to the d9 configuration, Cu(II) complexes are kinetically labile. BFCs for 62/64Cu-labeling are often macrocyclic and form Cu(II) complexes with high thermodynamic stability and kinetic inertness.61–76 Since most phosphonium cations are relatively small, the optimal BFCs would be those which form low molecular weight 64Cu chelates. That is why DO3A (1,4,7,10-tetraazacyclododecane-1,4,7-tetraacetic acid), DO2A (1,4,7,10-tetraazacyclododecane-1,4-diacetic acid), DOTA (1,4,7,10-tetraazacyclododecane-1,4,7,10-tetraacetic acid), and NOTA (1,4,7-tritazacyclononane-1,4,7-triacetic acid) are used as the BFCs for 64Cu-labeling of phosphonium cations.61–64 These BFCs are able to form anionic or neutral 64Cu chelates so that the overall molecular charge of the 64Cu radiotracers is either neutral or positive under physiological conditions.
Synthesis of Conjugated Organic Cations
DO3A conjugates were readily prepared according to Chart I by reacting the DO3A(OBu-t)3 with the respective bromide in DMF in the presence of sodium carbonate.61, 63, 64 Hydrolysis of the t-butyl ester in hydrochloric acid gave the expected DO3A conjugates (1: DO3A-pn-TPP; 2: DO3A-bn-TPP; 3: DO3A-xy-TPP; 4: DO3A-xy-TPA; 5: DO3A-xy-mTPP; and 6: DO3A-xy-TPEP). DO2A-xy-TPP (7) and DO2A-(xy-TPP)2 (8) were prepared according to Chart II by N-alkylation of DO2A(OBu-t)2 with 4-(bromomethylbenzyl)triphenylphosphonium.63 DOTA-Bn-xy-TPP (9), DOTA-Bn-xy-TPEP (10), NOTA-Bn-xy-TPP (11) and NOTA-Bn-xy-TPEP (12) were prepared according to Chart III.56 The key intermediates were (4-(aminomethyl)benzyl)(2-(diphenylphosphoryl)ethyl)diphenylphosphonium and 4-aminomethylbenzyl)triphenylphosphonium.63, 64 Conjugates 1 – 12 were synthesized to explore the impact of phosphonium moiety, linker and BFCs on the biodistribution and excretion kinetics of their corresponding 64Cu radiotracers.
Coordination Chemistry of DO3A-Conjugated TPP
Solid State Structures
To understand coordination chemistry of DO3A-conjugated phosphonium cations, we prepared complexes In(3)+ and Ga(3)+ as model compounds for 111In(3)+ and 68Ga(3)+, respectively, and Cu(3) as the model for 64Cu(3). Mn(3) was prepared because of its similarity to Cu(3) with respect to molecular charge.62 Despite their difference in overall molecular charge, In(3)+ and Mn(3) have almost identical solid state structures with DO3A bonding to In(III) and Mn(II) in a monocapped octahedral coordination geometry (Figure 2).62 Because of the smaller size of Ga(III), DO3A in Ga(3)+ is only hexadentate with four amine-N and two carboxylate-O atoms bonding to Ga(III) in a distorted octahedral coordination geometry (Figure 2). One carboxylic acid group in DO3A is deprotonated in order to balance the positive charge of Ga(III).62 Since the ionic radius of Cu(II) is close to that of Ga(III), it is reasonable to believe that the coordinated DO3A in Cu(3) is most likely hexadentate, as observed in Cu(DO3A),77 with one acetate group being deprotonated to balance the cationic charge from TPP.
Solution Structures
Since 64Cu(3) and 111In(3)+ are used as radiotracers in biological systems, it is necessary to study their solution properties (structure, isomerism and stability) in aqueous solution. On the basis of HPLC concordance experiments (Figure 3), it was concluded that 111In(3)+ and In(3)+ have the same composition due to their identical HPLC retention times.62 In(3)+ remains symmetrical in aqueous solution with no dissociation of acetate chelating arms.62 The presence of a single peak in the region of interest (Figure 3) suggests that they exist in solution as a single or “averaged” species. The HPLC retention times for In(3)+ and Ga(3)+ are almost identical (14.5 and 14.7 min, respectively); but they are significantly shorter than that of Mn(3) (16.8 min) and Cu(3) (17.2 min). Obviously, Ga(3)+ and In(3)+ with the +1 overall molecular charge are more hydrophilic than Mn(3) in its Zwitterion form.62 The HPLC retention time of Mn(3) (16.8 min) is close to that of Cu(3) (17.2 min) under identical chromatographic conditions (Figure 3), suggesting that Cu(3) may also exist in solution as its Zwitterion form.62–64 However, it is unclear if the two acetate chelating arms in 64Cu(3) remains coordinated in solution. Because of its low concentration in the blood circulation, it is quite possible that 64Cu-DO3A in 64Cu(3) might become 4-coordinated with a square planar coordination sphere. The lower pH value (pH = 4.5 – 5.0) inside tumor cells as compared to normal cells (pH = 6.5 – 7.4) also makes it easier for the two acetate chelating arms to become dissociated from 64Cu. This conclusion is supported by the fact that 64Cu(6) underwent extensive tranchelation in the liver,64 and completely consistent with the instability of the 64Cu-DOTA chelate.78–82
Biological Evaluation
Biodistribution Characteristics
More than 25 64Cu-labeled phosphonium cations have been evaluated for their biodistribution characteristics and excretion kinetics in athymic nude mice bearing U87MG human glioma xenografts.61, 63, 64 We were interested in this tumor-bearing animal model because the U87MG human glioma cell line has been used to evaluate the cellular uptake kinetics of 99mTc-Sestamibi and 99mTc-Tetrofosmin83 due to its lack of MDR1 P-glycoprotein (MDR1 Pgp) expression.84, 85 Western blotting studies also showed that the xenografted U87MG glioma tissues have little expression of MRP1, MRP2 and MRP4.65 Figure 4 compares 99mTc-Sestamibi and three 64Cu-labeled phosphonium cations for their uptake in the tumor, heart, liver and muscle, as well as tumor/heart and tumor/lung ratios. 99mTc-Sestamibi was used for comparison purposes since it has been clinically used for tumor imaging and monitoring of the tumor MDR transport function.36–42 The most striking difference is that all 64Cu radiotracers have the heart uptake <0.6% ID/g while the heart uptake of 99mTc-Sestamibi was >15% ID/g over the 2 h period. As a result, 64Cu radiotracers have the tumor/heart ratios much better than that of 99mTc-Sestamibi. The muscle uptake of 99mTc-Sestamibi was high (~5 %ID/g), whereas the muscle uptake of 64Cu radiotracers was almost undetectable at >30 min p.i. Thus, the 64Cu-labeled phosphonium cations have significant advantages over 99mTc-Sestamibi. The biodistribution of 64Cu(3) and 64Cu(4) was almost identical, suggesting the heteroatom (P vs. As) had very little impact on biodistribution of radiotracers.61 64Cu(3) has the tumor uptake comparable to that of 64Cu(5); but 64Cu(5) has the lower liver uptake, indicating that the presence of methoxy groups improves the radiotracer liver clearance.63 64Cu(6) had higher tumor uptake (Figure 4) than 64Cu(3), but its liver uptake was much lower than that of 64Cu(3).64 This indicates that the high liver uptake of 64Cu(3) is caused by TPP cation, not the in vivo instability of 64Cu-DO3A. On the basis of tumor uptake and T/B ratios (Figure 4), we believe that TPEP has better tumor-targeting capability than TPP.
Impact of BFC
The tumor uptake of 64Cu(10) is comparable to that of 64Cu(6) at 30 – 60 min p.i. (Figure 5A); but its tumor/heart ratios are lower than those of 64Cu(6), probably due to the benzene ring in 64Cu(10).64 Among 64Cu-labeled phosphonium cations evaluated in the glioma model, 64Cu(11) (Figure 5A) and 64Cu(12) (Figure 5B) had very low tumor uptake, probably due to NOTA,63, 64 which forms the Cu-NOTA chelate with better solution stability than that of Cu-DOTA.75 The extra xy-TPP moiety in 64Cu(8) also results in decreased tumor uptake (Figure 5B) and increased liver uptake, probably due to the +2 overall molecular charge and increased lipophilicity.64 On the basis of biodistribution data, it becomes clear that (1) DO3A is the best BFC for 64Cu-labeling of phosphonium cations; (2) NOTA-Bn has significant adverse effect on radiotracer tumor uptake; (3) DOTA derivatives might be useful BFCs if the aromatic benzene ring can be eliminated; and (4) the 64Cu chelate should have the neutral or negative charge. The combination of relatively high tumor uptake and high T/B ratios makes 64Cu(6) the most promising PET radiotracer for tumor imaging.63, 64
Impact of Metal Chelate
Figure 5C compares tumor uptake of 111In(3), 64Cu(3), 111In(6) and 64Cu(6). It is surprising that 64Cu and 111In radiotracers have such a significant difference in their tumor uptake. For example, both 64Cu(3) and 64Cu(6) have a steady increase in tumor uptake at 30 – 120 min p.i.63, 64 while 111In(3) and 111In(6) had a significant tumor washout over the 2 h study period. At this moment, it is not clear what causes the difference between 111In and 64Cu-labeled phosphonium cations. It seems that the radiotracers with an octahedral solution structure and high in vivo stability (111In-DO3A) tend to have much lower tumor uptake with shorter tumor retention time than those with a square-planar solution structure and relatively low in vivo stability (64Cu-DO3A). More studies are still in progress to further define the role of radiometal chelates on the tumor uptake and tumor retention time of radiolabeled phosphonium cations.
MicroPET Imaging
Figure 6 illustrates microPET images for 64Cu(2), 64Cu(3) and 64Cu(6) in athymic nude mice bearing U87MG glioma xenografts at 4 h p.i.61, 63, 64 The tumors were clearly visualized with excellent T/B contrast. It is interesting to note that the tumor uptake of 64Cu(2) was much lower than that of 64Cu(3), but its background radioactivity was also much lower.63 Therefore, all three 64Cu radiotracers are useful for imaging MDR-negative tumors by PET.
Metabolism and 64Cu-Transchelation in Liver
The metabolism studies showed that 64Cu(3) and 64Cu(6) are excreted via renal and hepatobiliary routes.61, 64 There was no significant metabolism detectable for 64Cu(6) in the feces sample at 120 min p.i. In contrast, only ~15% of 64Cu(3) remains intact in feces during the same study period. The radio-HPLC analysis of the liver homogenate suggest that 64Cu(6) underwent extensive 64Cu-tranchelation in the liver.64 While the identity of detected metabolites remains unknown, the radio-HPLC profile of 64Cu(6) is very similar to that of 64Cu-labeled TETA-Octreotide in rat liver homogenate.81 Thus, it is reasonable to believe that these metabolites are likely caused by 64Cu-transchelation from 64Cu-DO3A chelate to the proteins, such as superoxide dismutase (SOD), which are abundant in the liver.82
Stability of 64Cu-BFC Chelate and Radiotracer Liver uptake
Cu(II) has a d9 configuration with coordination number being 4, 5 or 6 depending on chelator. The 4-coordinated Cu(II) complexes are normally square-planar while the square-pyramid coordination geometry is often seen in 5-coordinated Cu(II) complexes. In 6-coordinated Cu(II) complexes, the two apical donor atoms are weakly bonded to Cu(II) in a distorted octahedral arrangement due to John-Teller distortion. As discussed previously, BFCs for copper radionuclides are often macrocyclic chelators that form Cu(II) complexes with high thermodynamic stability and kinetic inertness.55, 56 This was exemplified by early use of cyclam and cyclen derivatives for 67Cu-labeling of monoclonal antibodies,66 and further development of cross-bridged cyclam derivatives, such as CB-TE2A (2,2′-(1,4,8,11-tetraazabicyclo[6.6.2]hexadecane-4,11-diyl)diacetic acid).76, 78–80 It was reported that 64Cu-CB-TE2A had higher in vivo stability than 64Cu-DOTA and 64Cu-TETA.76, 78–80 Since Cu(II) complexes are kinetically labile due to its d9 configuration, the high liver uptake of 64Cu radiotracers is often attributed to their in vivo instability, which leads to 64Cu-transchelation from 64Cu-BFC to copper-binding proteins, such as superoxide dismutase abundant in liver.82 The metabolism of 64Cu-labeled biomolecules and 64Cu complexes of tetraazamacrocycles has been investigated extensively.66, 76, 78–80 These studies clearly show that kinetic inertness of 64Cu chelates is particularly important for in vivo stability of 64Cu radiotracers. However, the results from our studies suggested that the high radiotracer liver uptake is mainly caused by phosphonium cations, not instability of 64Cu-DO3A.61, 63, 64 This conclusion is supported by the fact that 64Cu(7) has significantly lower liver uptake than 64Cu(3) even though 64Cu-DO3A is expected to have better in vivo stability than 64Cu-DO2A.63 It is important to note that the tumor uptake of target-specific 64Cu radiotracers is almost exclusively determined by receptor binding of targeting biomolecules. The BFCs for 64Cu chelation should be those which form 64Cu-BFC chelates with high kinetic inertness to minimize liver radioactivity accumulation. In contrast, the optimal BFC should be those which result in the 64Cu radiotracer with high tumor uptake and the best T/B ratios since it has great impact on both tumor uptake and excretion kinetics of 64Cu-labeled phosphonium cations. From this point of view, DO3A and DOTA are suitable BFCs for 64Cu-labeling of phosphonium cations.
Tumor Localization Mechanism
Mitochondrial Potential: Driving Force for Tumor Localization
It is believed that mitochondrial potential is a major factor contributing to the tumor uptake of cationic radiotracers.3, 13, 46, 47, 52 Various tumor cell lines exhibit differences in the number, size and shape of their mitochondria relative to normal control cells.4 It has been reported that the mitochondria of rapidly growing tumors tend to be fewer in number and have fewer cristae than those from slowly growing tumors; the latter are larger and have characteristics closely resembling those of normal cells.4 The main difference between tumor cells and normal cells is mitochondrial potential (163 mV in carcinoma tumor cells vs. 104 mV in normal cells).7–10 According to the Nernst equation, the ~60 mV increase in mitochondrial potential will result in approximately 10-fold more accumulation of cationic compounds in the energized mitochondria of tumor cells (Figure 7). It is this mitochondrial potential difference that provides the contrast (differential uptake of radiotracer) between tumor and surrounding normal tissues. In addition, the plasma potential (−30 – −60 mV) also pre-concentrates cationic species relative to the external medium, thus affecting their cytoplasma concentration and availability for the mitochondrial uptake.13, 86–88
Activation Energy: Barrier to Across Lipid Membranes
Lipophilic cations, such as TPPs, are lipid-soluble despite their positive charge. They can readily pass through the phospholipid bilayer into the mitochondria.13 In contrast, hydrophilic cations, such as Na+ and K+, can across the plasma and mitochondrial transmembranes only with the help of ionophores or carrier proteins. The impermeability of biological membranes to hydrophilic cations is largely due to the high activation energy required to move them from an aqueous environment into the lipid core (Figure 8) of the membrane.86 The activation energy is composed of two components: the repulsive electrostatic interactions and the attractive hydrophobic forces.87 The main repulsive electrostatic energy component, Born energy, is due to the enthalpy required to overcome charge repulsion and to remove salvation water molecules from the cation upon transfer from aqueous environment to the lipid core of the membrane.13, 88 The Born energy (WB) is given by the following equation:
where εo is the vacuum permittivity, ε1 is the dielectric constant within the lipid core of the membrane (~2), ε2 is the dielectric of water (~80), q is the charge per mole of cation, r is the ionic radius, and Z is the charge per cation.13, 88 Born energy is decreased when cation becomes bigger (larger r value). The attractive component of activation energy is due to hydrophobicity of the cation (Figure 8). This energy is required to move an uncharged molecule with identical size and hydrophobicity from aqueous environment into lipid core of the phospholipid bilayer.86, 87 This component of activation energy is attractive for lipophilic organic cations due to increased entropy (loss of water structure when moving a molecule into the lipid core). The combination of decreased Born energy due to their much larger size and high attractive hydrophobic effect might contribute to 107 – 108-fold faster permeation kinetics through the phospholipid bilayer for triphenylphosphonium cations (Figure 9) as compared to that of Na+ and K+.87, 89
Membrane Penetration Kinetics: Control of Tumor Selectivity
Another important factor influencing the radiotracer’s tumor uptake and selectivity is mitochondrial density in different organs or tissues. Myocardium has the highest mitochondrial density and may occupy up to 40% of total volume of myocytes. Other mitochondrion-rich organs also include the salivary gland, liver and kidneys. For lipophilic cationic radiotracers (log P = 0.5 – 1.5), such as 99mTc-Sestamibi (log P = 1.1), their membrane diffusion kinetics are so fast that they tend to localize in the mitochondrion-rich organs, such as heart, liver, kidneys and salivary gland. For hydrophilic cations (log P = −1.0 – −3.0), such as 64Cu(6) (log P = −1.7), the low lipophilicity makes it more difficult for them to across mitochondrial membranes,63, 64 and often leads to a slow membrane diffusion kinetics; thereby forcing them to localize in tissues where the negative mitochondrial potential is elevated. Thus, it is not surprising that 64Cu(6) (log P = −1.7) and 64Cu(3) (log P = −2.7) have excellent tumor selectivity (Figure 9) with very low uptake in the heart and muscle. In this respect, cationic radiotracers with log P values in the range of 0.5 – 1.3 are particularly useful for imaging organs (heart, liver and salivary gland) with high mitochondrial density due to their fast membrane-penetration kinetics. In contrast, cationic radiotracers with log P values in the range of −1.0 to −3.0 are best fitted for imaging tumors with the elevated mitochondrial potential. This conclusion is completely consistent with the results from pre-clinical studies on cationic anticancer drugs and triarylmethane dyes for their phototoxicity towards tumor cells.90–94
Optimal Lipophilicity
There is little information available with regard to the optimal lipophilicity for a radiotracer to achieve high tumor-selectivity. A predictive model has been reported for selective accumulation of generic chemicals in carcinoma tumor cells.95 It was predicted that the optimal log P value for an organic cation to achieve high tumor selectivity is between 0.0 and −1.5. However, caution must be taken in using this predictive model because the molecular shape of 64Cu-labeled cations is significantly different from that of their parent phosphonium cations. Based on the results from biodistribution studies in the glioma model, it seems that the optimal log P value for a 64Cu-labeled phosphonium cation to achieve high tumor selectivity is between −1.0 and −3.0 (Figure 9). This conclusion should be further confirmed for other 64Cu-labeled organic cations.
Subcellular Distribution Characteristics
To understand the tumor localization mechanism of 64Cu-labeled phosphonium cations, subcellular distribution studies were performed on 64Cu(3) and 64Cu(6) using a standard differential centrifugation method.63, 64 99mTc-Sestamibi was used for comparison purposes since 99mTc-Sestamibi is widely used for imaging tumors in cancer patients. It was found that 64Cu(3), 64Cu(6) and 99mTc-Sestamibi share similar subcellular distribution patterns.63, 64 Since it is well-accepted that 99mTc-Sestamibi is a mitochondrion-targeting cationic radiotracer, we believe that 64Cu(3) and 64Cu(6) are able to localize in the energized mitochondria of tumor cells, where the negative potential is significantly elevated.
64Cu(DO3A-xy-ACR): A Close “Relative” of 64Cu-Labeled Phosphonium Cations
To further demonstrate the mitochondrion-targeting capability of 64Cu-labeled phosphonium cations, we recently evaluated 64Cu(DO3A-xy-ACR) (Figure 10: DO3A-xy-ACR = 2,6-bis(dimethylamino)-10-(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclo-dodecan-1-yl)methyl)benzyl)acridin-10-ium) in the glioma-bearing animal model.96 We also prepared Cu(DO3A-xy-ACR) for cell-staining assays. We found that 64Cu(DO3A-xy-ACR) remained in the glioma for >24 h while Cu(DO3A-xy-ACR) was able to localize in the mitochondria of glioma cells (Figure 10). Although 64Cu(DO3A-xy-ACR) is not an ideal PET radiotracer for tumor imaging due to its high liver uptake,96 the results from this study provided strong indirect evidence to suggest that 64Cu-labeled phosphonium cations are able to localize in the energized mitochondria of tumor cells, where the negative transmembrane potential is elevated.
Conclusion
64Cu-labeled phosphonium cations are a new class of PET radiotracers with high tumor selectivity. While their high tumor uptake can be attributed to the enhanced mitochondrial potential, the tumor selectivity of 64Cu-labeled phosphonium cations is most likely attributed to their low lipophilicity, and slow membrane-penetration kinetics. It is appreciated that 18F-labeling of phosphonium cations usually results in minimal changes in their physical and biological properties. In contrast, the radiolabeling of phosphonium cations with metallic radionuclide (such as 64Cu, 99mTc and 111In) requires the use of a BFC and results in significant changes in the molecular size, lipophilicity and biodistribution properties. Even though the exact structural requirements for radiometal chelates remain unknown, one thing is certain that attachment of the 64Cu-DO3A chelate onto phosphonium cations results in radiotracers with good tumor uptake and high tumor selectivity. Among the 64Cu-labeled phosphonium cations evaluated in the glioma-bearing animal model, 64Cu(6) has the best tumor uptake with very high tumor selectivity. Future studies will be directed towards understanding of solution structures of radiometal (64Cu, 99mTc and 111In) chelates and their impact on cellular uptake kinetics of radiolabeled phosphonium cations.
Acknowledgments
The author would like to thank Dr. Xiaoyuan Chen at the National Institute of Biomedical Imaging and Bioengineering (NIBIB) for PET imaging studies. This work is supported, in part, by Purdue University and research grants: R01 CA115883 from National Cancer Institute (NCI).
ABBREVIATIONS
- DO3A-bu-TPP (1)
triphenyl(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)-3-propyl)phosphonium
- DO3A-bu-TPP (2)
triphenyl(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)-4-butyl)phosphonium
- DO3A-xy-TPP (3)
triphenyl(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)benzyl)phosphonium
- DO3A-xy-TPA (4)
triphenyl(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)benzyl)arsonium
- DO3A-xy-mTPP (5)
tris(4-methoxyphenyl)(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)benzyl)phosphonium
- DO3A-xy-TPEP (6)
(2-(diphenylphosphoryl)ethyl)diphenyl(4-((4,7,10-tris(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)benzyl)phosphonium
- DO2A-xy-TPP (7)
(4-((4,10-bis(carboxymethyl)-1,4,7,10-tetraazacyclododecan-1-yl)methyl)benzyl)triphenylphosphonium
- DO2A-(xy-TPP)2 (8)
(4,4′-(4,10-bis(carboxymethyl)-1,4,7,10-tetraazacyclododecane-1,7-diyl)bis(methylene)bis(4,1-phenylene))bis(methylene)bis(triphenylphosphonium)
- NOTA-Bn-xy-TPP (9)
triphenyl(4-((3-(4-((1,4,7,10-tetrakis(carboxymethyl)-1,4,7,10-tetraazacyclododecan-2-yl)methyl)phenyl)thioureido)methyl)benzyl)phosphonium
- DOTA-Bn-xy-TPEP (10)
(2-(diphenylphosphoryl)ethyl)diphenyl(4-((3-(4-((1,4,7,10-tetrakis(carboxymethyl)-1,4,7,10-tetraazacyclododecan-2-yl)methyl)phenyl)thioureido)methyl)benzyl)phosphonium
- NOTA-Bn-xy-TPEP (11)
(2-(diphenylphosphoryl)ethyl)diphenyl(4-((3-(4-((1,4,7-tris(carboxymethyl)-1,4,7-triazonan-2-yl)methyl)phenyl)thioureido)methyl)benzyl)phosphonium
- and NOTA-Bn-xy-TPP (12)
triphenyl(4-((3-(4-((1,4,7-tris(carboxymethyl)-1,4,7-triazonan-2-yl)methyl)phenyl)thioureido)methyl)benzyl)phosphonium
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