Hefei National Research Center for Physical Sciences at the Microscale, CAS Key Laboratory of Soft Matter Chemistry, School of Chemistry and Materials Science, University of Science and Technology of China, Hefei 230026, China
Xu Chen is currently pursuing a master’s degree at the University of Science and Technology of China. His research focuses on the application of nanomaterials in the biological field
Feng Gao received his Ph.D. degree in Materials Science and Engineering from the University of Science and Technology of China (USTC) in 2021. Currently, he is a postdoctoral fellow at USTC. His research focuses on the preparation of biomaterials and their applications in antibacterial and artificial carbon cycling
Lihua Yang received her Ph.D. degree from the University of Illinois at Urbana Champaign in 2008. She is currently an Associate Professor at the University of Science and Technology of China. Her research mainly focuses on the application of nanomaterials in the biological field
To make small molecular photosensitizer-based nanoparticles photostable, we polymerized such photosensitizers via emulsion polymerization, and the resulting nanoparticles exhibited sustained absorption of the excitation wavelength in the near-infrared region, generated stable photothermal and photodynamic effects upon repeated irradiation with an near-infrared laser, and efficiently eradicated cancerous cells even after prior irradiation exposure.
Graphical Abstract
Synthesis route of CSNP and characterization of its photothermal properties.
Abstract
To make small molecular photosensitizer-based nanoparticles photostable, we polymerized such photosensitizers via emulsion polymerization, and the resulting nanoparticles exhibited sustained absorption of the excitation wavelength in the near-infrared region, generated stable photothermal and photodynamic effects upon repeated irradiation with an near-infrared laser, and efficiently eradicated cancerous cells even after prior irradiation exposure.
Public Summary
In order to improve the loading rate of photosensitizer, small molecular dyes were polymerized into nanoparticles by emulsion polymerization, and their photostability was improved by ensuring high loading efficiency of photosensitizer.
The experimental results show that Cypate nanosphere (CyNS) shows good colloidal stability in PBS and continuous absorption of excitation light.
After repeated light irradiation, CyNS significantly enhances the stability of photothermal and photodynamic effects, which can lead to a significant improvement in the efficacy of cancer phototherapy with repeated light irradiation.
As the development of science and technology, some data sets are recorded frequently with curves, surfaces and other types, which are usually called functional data that plays an important role in wide fields such as atmospheric science, engineering, medical research, see more details in Ramsay and Silverman[1]. Functional regression models are useful tools in functional data analysis, where one of the most interesting and challenging cases is function-on-function regression, see Ramsay and Silverman[1,2], Yao et al.[3, 4]. In this paper, we consider the following functional model proposed by Wang et al.[5], for m=1,⋯,M,
where ym(t) is the functional response, zm(t) is a p-vector of functional covariates, ν is the corresponding parameters, xm(s,t) is a q-dimensional of covariates depends on s and t, and β(s,t) is a vector of the functional coefficients, St is interval for t, εm(t) is random error term for the mth curve. Model (1) is flexible, and includes some function-on-function models in Gervini[6], Malfait and Ramsay[7], Ramsay and Silverman[2], as special cases. Note that τm is used to model the heterogeneity among the different subjects, which depends on zm(t), xm(⋅,t). Wang et al.[5] considered the above random effects model using Gaussian process priors. More on Gaussian process priors in functional model[8,9].
However, when there exist outliers in the observations, it is not robust to use the model based on Gaussian process priors, see e.g. Wang et al.[10]. Then in order to overcome the influence of outliers, various forms of student t-process have been developed to model a heavy-tailed process, e.g. Yu et al.[11], Zhang and Yeung[12]. Shah et al.[13] pointed out that the t-distribution under addition is not closed to maintain the good properties of Gaussian models. Thus, Wang et al.[10] developed an extended t-process regression, which has the following advantages: ① it can maintain the good properties of Gaussian process; ② it has flexible forms, and contains model in Shah et al.[13] as a special case; ③ it is robust. More general discussions on t-process can see Refs. [10,14].
In this paper, we consider a functional nonparametric random effects model with extended t-process priors, and propose an estimation procedure. The proposed method has 3 merits. ① It applies the extended t-process prior to model the heterogeneity of individual effect in the function-on-function regression model such that the model has robustness; ② A basis expansion smoothing method and a penalized likelihood method are developed to estimate the parameter in the fixed effect and covariance function of random effects, which leads to estimation of the smoothing function and prediction of the random effect; ③ Information consistency of the parameter estimation is obtained.
The remainder of the paper is organized as follows. In Section 2, we present the nonparametric random effects model using extended t-process priors, and develop prediction distribution and estimation procedure. In Section 3, we conduct simulation studies and a real data example to evaluate the performance of the proposed method. The conclusions are given in Section 4. All the proofs are given in Appendix.
2.
Main results
2.1
Extended t-process
Extended t-process proposed by Wang et al.[10] is briefly introduced as follows. Let f(⋅), a real-valued random function from X to R, satisfy that
f∣r∼GP(h,rk),r∼IG(v,ω),
where GP(⋅,⋅) and IG(⋅,⋅) stand for Gaussian process and inverse gamma distribution respectively. Then f follows an extended t-process (ETP), and can be denoted by f∼ETP(v,ω,h,k). We call h(⋅):X→R mean function and k(⋅,⋅):X×X→R covariance kernel function. From the definition of ETP, we show that for any points X=(x1,⋯,xn)⊤, we have
fn=f(X)=(f(x1),⋯,f(xn))⊤∼EMTD(ν,ω,hn,Kn),
meaning that fn has an extended multivariate t-distribution (EMTD) with the following density function,
where hn=(h(x1),⋯,h(xn))⊤,Kn=(kij)n×n and kij=k(xi,xj).
2.2
Function-on-function regression model with random effects
In model (1), the random effect τm depicts individual effect. Considering robustness against outliers, an ETP process prior is applied to τm. This paper assumes that τm and εm have a joint extended t-process,
(τmεm)∼ETP(v,ω,(00),(k00σ2δε)),
where δε(t,s)=I(t=s) and I(⋅) is an indicator function.
Note that the random effect τm relies on zm(t) and xm(⋅,t), then following Wang et al.[5], the kernel function k is an expression as
where um(t)=(z⊤m(t),x⊤m(⋅,t))⊤, zm(t)=(zm1(t),⋯,zmp(t))⊤ and xm(s,t)=(xm1(s,t),⋯,xmq(s,t))⊤. Let θ=(θ10,θ11,⋯,θ1Q,θ21,⋯,θ2Q)⊤ represent a set of hyper-parameters with Q=p+q, and ‖g(⋅)‖Λ be a Λ norm of function g. A choice of ‖⋅‖Λ is the L2 norm of a function, that is, ‖g(⋅)‖Λ=∫g(s)2ds is a Λ norm of function g.
Let observations {ymi=ym(ti), i=1,⋯,n,m=1,⋯,M}, um(ti)=(z⊤m(ti),x⊤m(⋅,ti))⊤, error term εmi=εm(ti), where {ti} are observed times. Assume that true values of ν, β, τm in model (1) are ν0, β0, τ0m respectively. From model (1), we further consider the following (true) data model:
where ym=(ym(t1),⋯,ym(tn))⊤ are observations for the mth subject at points {t1,⋯,tn}, similarly, τm=(τm(um(t1)),⋯,τm(um(tn)))⊤, cm=(cm(t1),⋯,cm(tn))⊤, Km=(kθ(um(ti),um(tj)))n×n, I is the identity matrix.
Denoted by the data set D={(ym(tj),um(tj)):j=1,⋯,n,m=1,⋯,M}. Since that
(ymτm)|um∼ETMD(v,w,(c⊤m,0⊤)⊤,(Km+σ2IKmKmKm)),
we obtain the posterior distribution of τm, that is
where Λ=diag(0p×p,λsJψψ⊗Lϕϕ+λtLψψ⊗Jϕϕ,⋯,λsJψψ⊗Lϕϕ+λtLψψ⊗Jϕϕ) is a (p+qKsKt)×(p+qKsKt) matrix. Similarly, we can get estimation equations with respect to θ and σ2.
From these estimation equations, we construct an estimation procedure as follows.
Step 1 Given an initial estimate of θ;
Step 2 Given θ, we update the estimates of b and σ2 via
argmin
Step 3 Given {\boldsymbol{b}} and \sigma^2 , we update the estimate of {\boldsymbol{\theta}} via
Step 4 Repeat Step 2 and Step 3 until convergence.
Similar to Ref. [5], when the absolute value of relative difference of l({\boldsymbol{{\theta}}}, {\boldsymbol{{b}}}, \sigma^{2}) between two successive iterations is less than a given value, the procedure stops.
2.5
Information consistency
The common mean structure and its properties have been studied a lot in functional models, see Yao et al.[4], Yuan and Cai[15], Sun et al.[16], and among others. Next we only consider the information consistency. Let {\cal {X}}={\cal {X}}_1 \times {\cal{X}}_2 , where {\cal {X}}_1 and {\cal{X}}_2 are spaces covariates {\boldsymbol{z}}_{m}(t) and {\boldsymbol{x}}_{m}(\cdot,t) belonging to. Let p_{\sigma _{0}}({\boldsymbol{{y}}}_{{m}}|\tau_{0m},{\boldsymbol{{u}}}_{{m}}) be the density function to generate the data {\boldsymbol{{y}}}_{{m}} given {\boldsymbol{{u}}}_{{m}} and \tau_{0m} , where \sigma_{0} is the true value of \sigma , \tau_{0m} is the true value of \tau_m . Let p_{{\boldsymbol{{\theta}}}}(\tau) be a measurement of the random process \tau on space \cal{F}=\{\tau(\cdot,\cdot): {\cal{X}} \rightarrow R\} . Let
be the density function to generate the data {\boldsymbol{{y}}}_{{m}} given {\boldsymbol{{u}}}_m under model (1). Let p_{\sigma_0,\hat{{\boldsymbol{\theta }}}}({\boldsymbol{{y}}}_{{m}}|{\boldsymbol{{u}}}_{{m}}) be the estimated density function. Denote
as the Kullback-Leibler divergence between two densities p_{1} and p_{2} . According to Ref. [6], we only need to show the Kullback-Leibler divergence between two density functions for {\boldsymbol{{y}}}_{{m}}|{\boldsymbol{{u}}}_{{m}} from the true and the assumed models tends to zero when n is large enough.
For information consistency of the parameter estimation, we need the following condition.
where \|\tau_{0m}\|_k is the reproducing kernel Hilbert space norm of \tau_{0m} associated with k(\cdot , \cdot ;{\boldsymbol{{\theta}}}) , {\boldsymbol{{K}}}_{{m}} is covariance matrix of \tau_{0m} over {\boldsymbol{{u}}}_{{m}} , {\boldsymbol{{I}}} is the n \times n identity matrix.
More details about Condition (A) can see Seeger et al.[17] and Wang et al.[5]. More on reproducing kernel Hilbert space can see Berlinet and Thomas[18].
Proposition 2.1. Under the conditions in Lemma A.1 (Appendix) and condition (A), we have
\begin{array}{l} \dfrac{1}{n} E_{{\boldsymbol{{u}}}_{{m}}}\left(D[p_{\sigma _{0}}({\boldsymbol{{y}}}_{{m}}|\tau_{0m},{\boldsymbol{{u}}}_{{m}}),p_{\sigma_0,\hat{\boldsymbol{{\theta }}}}({\boldsymbol{{y}}}_{{m}}|{\boldsymbol{{u}}}_{{m}})]\right) \longrightarrow 0, \quad {\rm { as }} \quad n \rightarrow \infty, \end{array}
where the expectation is taken over the distribution of {\boldsymbol{{u}}}_{{m}} .
3.
Numerical results
3.1
Simulations
Performance of the proposed method is investigated by numerical studies. Simulation data are generated by the following model,
where {z}_{m}(\cdot) \sim {\rm{GP}}(h_1, k_1), h_1 = h_1(t) = t , for t \in (0,1) , k_1 = k_1({z}_{m}(t_1), {z}_{m}(t_2)) \;=\; g(t_1,t_2) \;=\; 0.1\exp\{-5(t_1-t_2)^2\} + 0.1t_1t_2, and {x}_{m} (\cdot,\cdot) \sim GP(h_2, k_2), h_2 = h_2(t) = t + {\rm{cos}}(s)(s), for t,s \in (0,1) , k_2 = k_2({x}_{m}(s_1,t),{x}_{m}(s_2,t)) = g(s_1,s_2). Let {\boldsymbol{{\nu}}} = 1.0, \theta_{10} = \theta_{12} =\theta_{21} = \theta_{22} = 0.1, \theta_{11} = 10, \sigma^2 = 0.5 , and t and s take 20 points equally in (0,1). Consider four different combinations of \tau_{m} and {\boldsymbol{{\beta}}}(s,t) ,
S1: \tau_{m} \sim {\rm{GP}}(0, {\rm Cov}(\tau_{m}({\boldsymbol{{u}}}_{{m}}(t_{1})), \tau_{m}({\boldsymbol{{u}}}_{{m}}(t_{2})))), and h_2 = h_2(t) = t +{\rm{cos}}(s) (s), for s,t \in (0,1) ;
S2: \tau_{m} \sim {\rm{GP}}(0, {\rm Cov}(\tau_{m}({\boldsymbol{{u}}}_{{m}}(t_{1})), \tau_{m}({\boldsymbol{{u}}}_{{m}}(t_{2})))), and {\boldsymbol{{\beta}}}(s,t) \;=\; \exp \{-(t^2 + s^2)\}/10, for s,t \in (0,1) ;
S3: \tau_{m} =0 and {\boldsymbol{{\beta}}}(s,t) = (t^2 + \cos(s))/10 , for s,t \in (0,1) ;
S4: \tau_{m} =0 and {\boldsymbol{{\beta}}}(s,t) = \exp\{-(t^2 + s^2)\}/10 , for s,t \in (0,1) .
We take sample sizes M =10, 20, and 30. All simulations are repeated 500 times.
To show robustness of model (1) with random effect having ETPR, saying ETPR, we also compute model (1) with random effect having GPR, denoted by GPR. Two indices: prediction error (PE),
are applied to show performance of two methods: ETPR and GPR, where \hat{f}(t)={\boldsymbol{{z}}}_{{m}}^{{\top}}(t)\hat{{\boldsymbol{{\nu}}}}+\int_{0}^{1} {\boldsymbol{{x}}}_{{m}}^{{\top}}(s,t)\hat{{\boldsymbol{{\beta}}}}(s,t){\rm{d}}s+ \hat{\tau}_{m}({\boldsymbol{{z}}}_{{m}}(t), {\boldsymbol{{x}}}_{{m}}(\cdot, t)) is an estimator of the true regression function f_0(t)= {\boldsymbol{{z}}}_{{m}}^{{\top}}(t){\boldsymbol{{\nu}}}_0+\int_{0}^{1} {\boldsymbol{{x}}}_{{m}}^{{\top}}(s,t){\boldsymbol{{\beta}}}_0(s,t){\rm{d}}s+\tau_{0m}({\boldsymbol{{z}}}_{{m}}(t), {\boldsymbol{{x}}}_{{m}}(\cdot, t)). To show robustness of our method, one curve is randomly selected and added with an extra disturbance, \delta t_3 , where t_3 stands for student t distribution with degree of freedom 3. Table 1 presents the values of PE and AB from these two methods. We see that ETPR has smaller PE and AB than GPR, especially with \delta = 1.0 and small sample sizes. It shows that the proposed method ETPR has more robustness against outliers compared to GPR.
Table
1.
PE and AB of prediction from ETPR method and GPR method, where SDs are presented in parentheses.
In addition, we also consider one constant disturbance for the abnormal curves with small sample sizes 10 and 20. Tables 2 and 3 present PE and AB of prediction from ETPR method and GPR method for one and two curves disturbed, respectively. We see that ETPR has better performance in prediction compared to GPR.
Table
2.
PE and AB of prediction from ETPR method and GPR method with one curve disturbed by constant 1.0, where SDs are presented in parentheses.
The proposed method is applied to Canadian weather data, which is obtained from the R package fda. We aim to study fixed effect of temperature on precipitation by common temperature effect of stations in the same region, and random effect of temperature on precipitation by individual effect of each station. Generally, the 35 stations are divided into four regions: Arctic, Atlantic, Pacific and Continental. Obviously, there exists heterogeneity among the stations due to the spatial nature of the weather data. Then we propose the following model:
where {y}_{ij}(t) represents precipitation and {x}_{ij}(t) represents temperature, for time t , region i and j th station. In this model, we have {z}_{ij}(t) = 1 and {x}_{ij}(s,t) = {x}_{ij}(s) which effectively simplifies model fit.
Figs. 1 and 2 show random and fixed effects of the 4 regions: Arctic, Atlantic, Pacific and Continental from the proposed method. We see from the random effects that each station in the same region has different temperature effects on the precipitation. To compare performance of prediction from ETPR with GPR, 10-folds cross validation method is used to compute mean squares of prediction errors, 0.310 and 0.314, for ETPR and GPR, respectively. It shows that ETPR has a little better performance in prediction.
Figure
1.
Random and fixed effects of model using ETPR for Arctic and Atlantic.
A function-on-function random effects model with extended t-process prior in this paper is developed to analyze functional data which may include outliers. The proposed model is flexible, including various kinds of functional models, such as the function-on-function linear model[2] and the historical functional regression model[7] as special cases. The proposed extended t-process model is not only robust against outliers, but also inherits almost all the nice properties from Gaussian process regression, such as closed form of prediction and convenient computation procedure. The estimation procedure and computing algorithm are developed to estimate the parameters and predict the random effect in the regression model. The functional response considered in this paper has one dimension. In practical application, functional multi-response may consist of several correlated curves. It is interesting that the proposed method is extended to functional data with multi-response, which will be studied in our further work.
Appendix
Lemma A.1. Let w=v-1 . Under model (1), assume that {\boldsymbol{{y}}}_{{m}} are independently sampled, the covariance kernel function k is bounded and continuous on the parameter {\boldsymbol{{\theta}}} , and \hat{{\boldsymbol{\theta}}} converges to {\boldsymbol{{\theta}}} when n \rightarrow \infty . Then, for a positive constant c and any \varepsilon>0 , when n is large enough, we have
where q_m^{2}=({\boldsymbol{{y}}}_m-{\boldsymbol{{c}}}_{{0m}}-{\boldsymbol{{\tau}}}_{{0m}})^{\top}({\boldsymbol{{y}}}_{{m}}-{\boldsymbol{{c}}}_{{0m}}-{\boldsymbol{{\tau}}}_{{0m}}) / \sigma_{0}^2 , {\boldsymbol{{c}}}_{{0m}} is the true value of {\boldsymbol{{c}}}_{{m}} , \|\tau_{0m}\|_k is the reproducing kernel Hilbert space norm of \tau_{0m} associated with k(\cdot , \cdot ;{\boldsymbol{{\theta}}}) , {\boldsymbol{{K}}}_{{m}} is covariance matrix of \tau_{0m} over {\boldsymbol{{u}}}_{{m}} , {\boldsymbol{{I}}} is the n \times n identity matrix.
Proof of Lemma A.1. Assume r is a random variable following inverse gamma distribution {\rm{IG}}(v,(v-1)). Conditional on r , we have
where {\rm{GP}}(h,k) stands for Gaussian process with mean function h and covariance function k . Then conditional on r_m , the extended t-process regression model y_m=c_m+\tau_m+\varepsilon_m becomes Gaussian process regression model
where \tilde{\tau}_m=\tau_m|r_m \sim {\rm{G P}}(0, r_m k(\cdot, \cdot; {\boldsymbol{\theta}})), \tilde{\varepsilon}_m=\varepsilon_m| r_m \sim {\rm{G P}}(0, r \sigma^2\delta_{\varepsilon}), and \tilde{\tau}_m and \tilde{\varepsilon}_m are independent. Denoted the computation of conditional probability density for given r_m by \tilde{p} . Let
where \tilde{p}_{\boldsymbol{\theta}} is the induced measure from Gaussian process {\rm{G P}}(0, r_m k(\cdot,\cdot ; \hat{\boldsymbol{\theta}})). Note that variable r is independent of {\boldsymbol{{u}}}_{{m}} . We can show that
Proof of Proposition 2.1. Obviously q_m^{2}=({\boldsymbol{{y}}}_m-{\boldsymbol{{c}}}_{{0m}}-{\boldsymbol{{\tau}}}_{{0m}})^{\top} \cdot ({\boldsymbol{{y}}}_m-{\boldsymbol{{c}}}_{{0m}}-{\boldsymbol{{\tau}}}_{{0m}}) / \sigma_{0}^2=O(n). Under the conditions of Lemma A.1 and condition (A), by Lemma A.1, for a positive constant c and any \varepsilon>0 , when n is large enough, we have
We thank the reviewers for their insightful comments and suggestions. This work was supported in part by the National Natural Science Foundation of China (11971457), Anhui Provincial Natural Science Foundation (1908085MA06) and the Fundamental Research Funds for the Central Universities (WK2040000035).
Conflict of interest
The authors declare that they have no conflict of interest.
Acknowledgements
This work was supported by the Youth Innovation Promotion Association of the Chinese Academy of Sciences and the Ministry of Education of the People’s Republic of China (NCET-13-0547). We gratefully thank Professors Jun Wang and Zhishen Ge for use of their facilities. We also thank Lulu Xu and Jigang Piao for technical assistance.
Conflict of interest
The authors declare that they have no conflict of interest.
In order to improve the loading rate of photosensitizer, small molecular dyes were polymerized into nanoparticles by emulsion polymerization, and their photostability was improved by ensuring high loading efficiency of photosensitizer.
The experimental results show that Cypate nanosphere (CyNS) shows good colloidal stability in PBS and continuous absorption of excitation light.
After repeated light irradiation, CyNS significantly enhances the stability of photothermal and photodynamic effects, which can lead to a significant improvement in the efficacy of cancer phototherapy with repeated light irradiation.
Yuwen L H, Zhou J J, Zhang Y Q, et al. Aqueous phase preparation of ultrasmall MoSe2 nanodots for efficient photothermal therapy of cancer cells. Nanoscale,2016, 8 (5): 2720–2726. DOI: 10.1039/C5NR08166A
[2]
Huang P, Lin J, Li W W, et al. Biodegradable gold nanovesicles with an ultrastrong plasmonic coupling effect for photoacoustic imaging and photothermal therapy. Angew. Chem. Int. Edit.,2013, 52 (52): 13958–13964. DOI: 10.1002/anie.201308986
[3]
Tian B, Wang C, Zhang S, et al. Photothermally enhanced photodynamic therapy delivered by nano-graphene oxide. ACS Nano,2011, 5 (9): 7000–7009. DOI: 10.1021/nn201560b
[4]
Shi S G, Zhu X L, Zhao Z X, et al. Photothermally enhanced photodynamic therapy based on mesoporous Pd@Ag@mSiO2 nanocarriers. J. Mater. Chem. B.,2013, 1 (8): 1133–1141. DOI: 10.1039/c2tb00376g
[5]
Huang X H, El-Sayed I H, Qian W, et al. Cancer cell imaging and photothermal therapy in the near-infrared region by using gold nanorods. J. Am. Chem. Soc.,2006, 128 (6): 2115–2120. DOI: 10.1021/ja057254a
[6]
Nolsøe C P, S. Torp-Pedersen S, Burcharth F, et al. Interstitial hyperthermia of colorectal liver metastases with a US-guided Nd-YAG laser with a diffuser tip: A pilot clinical study. Radiology,1993, 187 (2): 333–337. DOI: 10.1148/radiology.187.2.8475269
[7]
Dolmans D E J G J, Fukumura D, Jain R K. Photodynamic therapy for cancer. Nat. Rev. Cancer,2003, 3 (5): 380–387. DOI: 10.1038/nrc1071
[8]
Piao J G, Wang L M, Gao F, et al. Erythrocyte membrane is an alternative coating to polyethylene glycol for prolonging the circulation lifetime of gold nanocages for photothermal therapy. ACS Nano,2014, 8 (10): 10414–10425. DOI: 10.1021/nn503779d
[9]
Chen H C, Tian J W, He W J, et al. H2O2-activatable and O2-evolving nanoparticles for highly efficient and selective photodynamic therapy against hypoxic tumor cells. J. Am. Chem. Soc.,2015, 137 (4): 1539–1547. DOI: 10.1021/ja511420n
[10]
Weissleder R. A clearer vision for in vivo imaging. Nat. Biotechnol.,2001, 19 (4): 316–317. DOI: 10.1038/86684
[11]
Weissleder R, Ntziachristos V. Shedding light onto live molecular targets. Nat. Med.,2003, 9 (1): 123–128. DOI: 10.1038/nm0103-123
[12]
Ma Z Y, Yang M K, Foda M F, et al. Polarization of tumor-associated macrophages promoted by vitamin C-loaded liposomes for cancer immunotherapy. ACS Nano,2022, 26 (10): 17389–17401. DOI: 10.1021/acsnano.2c08446
[13]
Wu L, Fang S T, Shi S, et al. Hybrid polypeptide micelles loading indocyanine green for tumor imaging and photothermal effect study. Biomacromolecules,2013, 14 (9): 3027–3033. DOI: 10.1021/bm400839b
[14]
Zheng X H, Xing D, Zhou F F, et al. Indocyanine green-containing nanostructure as near infrared dual-functional targeting probes for optical imaging and photothermal therapy. Mol. Pharmaceut.,2011, 8 (2): 447–456. DOI: 10.1021/mp100301t
[15]
Yu J, Javier D, Yaseen M A, et al. Self-assembly synthesis, tumor cell targeting, and photothermal capabilities of antibody-coated indocyanine green nanocapsules. J. Am. Chem. Soc.,2010, 132 (6): 1929–1938. DOI: 10.1021/ja908139y
[16]
Yang H, Mao H J, Wan Z H, et al. Micelles assembled with carbocyanine dyes for theranostic near-infrared fluorescent cancer imaging and photothermal therapy. Biomaterials,2013, 34 (36): 9124–9133. DOI: 10.1016/j.biomaterials.2013.08.022
[17]
Wang Y, Yang T, Ke H T, et al. Smart albumin-biomineralized nanocomposites for multimodal imaging and photothermal tumor ablation. Adv. Mater.,2015, 27 (26): 3874–3882. DOI: 10.1002/adma.201500229
[18]
Han Y, Li J J, Zan M H, et al. Redox-responsive core cross-linked micelles based on cypate and cisplatin prodrugs-conjugated block copolymers for synergistic photothermal–chemotherapy of cancer. Polym. Chem.,2014, 5 (11): 3707–3718. DOI: 10.1039/C4PY00064A
[19]
Zheng M B, Yue C X, Ma Y F, et al. Single-step assembly of DOX/ICG loaded lipid–polymer nanoparticles for highly effective chemo-photothermal combination therapy. ACS Nano,2013, 7 (3): 2056–2067. DOI: 10.1021/nn400334y
[20]
Li Y L, Deng Y B, Tian X, et al. Multipronged design of light-triggered nanoparticles to overcome cisplatin resistance for efficient ablation of resistant tumor. ACS Nano,2015, 9 (10): 9626–9637. DOI: 10.1021/acsnano.5b05097
[21]
Bugaj J E, Achilefu S I, Dorshow R B, et al. Novel fluorescent contrast agents for optical imaging of in vivo tumors based on a receptor-targeted dye-peptide conjugate platform. J. Biomed. Opt.,2001, 6 (2): 122–133. DOI: 10.1117/1.1352748
[22]
Ye Y P, Bloch S, Kao J, et al. Multivalent carbocyanine molecular probes: Synthesis and applications. Bioconjugate Chem.,2005, 16 (1): 51–61. DOI: 10.1021/bc049790i
[23]
Bourré L, Thibaut S, Briffaud A, et al. Indirect detection of photosensitizer ex vivo. J. Photochem. Photobiol. B,2002, 67 (1): 23–31. DOI: 10.1016/S1011-1344(02)00279-8
[24]
Yuan Y, Min Y, Hu Q, et al. NIR photoregulated chemo- and photodynamic cancer therapy based on conjugated polyelectrolyte–drug conjugate encapsulated upconversion nanoparticles. Nanoscale,2014, 6 (19): 11259–11272. DOI: 10.1039/C4NR03302G
[25]
Knop K, Hoogenboom R, Fischer D, et al. Poly(ethylene glycol) in drug delivery: Pros and cons as well as potential alternatives. Angew. Chem. Int. Ed.,2010, 49 (36): 6288–6308. DOI: 10.1002/anie.200902672
1.
Schematic illustration of the preparation of Cypate nanospheres (CyNSs), which are obtained by polymerizing the Cypate-HEA monomer, in which one carboxyl group of a Cypate molecule is esterified with 2-hydroxyethyl acrylate (HEA) via an emulsion polymerization process.
Figure
1.
(a) Transmission electron microscopy image of CyNS. Scale bar = 500 nm. (b) The average zeta potential of CyNS in aqueous solution. (c) The average hydrodynamic diameters of CyNS in 1×PBS over a span of 5 d. Data points are reported as the mean ± standard deviation. (d) Normalized absorbance ratios of CyNS (PS content of 10.0 μg/mL, 0.5 mL) at different time points during irradiation with an 808-nm laser at 1.0 W/cm2 for 15 min in total, with those of free Cypate included for comparison.
Figure
2.
(a) Cumulative heat generated by the dispersion of CyNS in PBS (PS content of 10 μg/mL, 400 μL) at different time points during the 1st, 2nd, 3rd, 4th, 5th, and 6th irradiation treatments (with an 808-nm laser at 1.0 W/cm2 for 10 min), with those of free Cypate in DMF included for comparison. \\: indicates natural cooling for 12 h. (b) Thermographs of mice injected with CyNS, free Cypate, or PBS during a 10-min irradiation (with an 808-nm laser at 1.0 W/cm2) immediately after injection. Mice assayed similarly but injected with PBS only are included as a reference. (c) Plots of temperature change at the tumor site as a function of irradiation time based on thermographs. Data points are reported as the mean ± standard deviation (n=3). ** indicates p< 0.01. (d) Fluorescence emission spectra of dichlorofluorescein hydrolysate (DCFH) in dispersions of CyNS in PBS and Cypate in methanol after the 1st, 2nd, 3rd, and 4th treatments. \\: natural cooling for 2 min.
Figure
3.
In vitro cell viability assays using free Cy/pretreated Cy and CyNS/pretreated CyNS incubated with HeLa cells for 24 h with 10 min of irradiation (808 nm, 1.0 W/cm2). Controls are culture medium irradiated similarly with an 808-nm laser at 1.0 W/cm2. Data points are reported as the mean ± standard deviation. ** indicates p < 0.01.
References
[1]
Yuwen L H, Zhou J J, Zhang Y Q, et al. Aqueous phase preparation of ultrasmall MoSe2 nanodots for efficient photothermal therapy of cancer cells. Nanoscale,2016, 8 (5): 2720–2726. DOI: 10.1039/C5NR08166A
[2]
Huang P, Lin J, Li W W, et al. Biodegradable gold nanovesicles with an ultrastrong plasmonic coupling effect for photoacoustic imaging and photothermal therapy. Angew. Chem. Int. Edit.,2013, 52 (52): 13958–13964. DOI: 10.1002/anie.201308986
[3]
Tian B, Wang C, Zhang S, et al. Photothermally enhanced photodynamic therapy delivered by nano-graphene oxide. ACS Nano,2011, 5 (9): 7000–7009. DOI: 10.1021/nn201560b
[4]
Shi S G, Zhu X L, Zhao Z X, et al. Photothermally enhanced photodynamic therapy based on mesoporous Pd@Ag@mSiO2 nanocarriers. J. Mater. Chem. B.,2013, 1 (8): 1133–1141. DOI: 10.1039/c2tb00376g
[5]
Huang X H, El-Sayed I H, Qian W, et al. Cancer cell imaging and photothermal therapy in the near-infrared region by using gold nanorods. J. Am. Chem. Soc.,2006, 128 (6): 2115–2120. DOI: 10.1021/ja057254a
[6]
Nolsøe C P, S. Torp-Pedersen S, Burcharth F, et al. Interstitial hyperthermia of colorectal liver metastases with a US-guided Nd-YAG laser with a diffuser tip: A pilot clinical study. Radiology,1993, 187 (2): 333–337. DOI: 10.1148/radiology.187.2.8475269
[7]
Dolmans D E J G J, Fukumura D, Jain R K. Photodynamic therapy for cancer. Nat. Rev. Cancer,2003, 3 (5): 380–387. DOI: 10.1038/nrc1071
[8]
Piao J G, Wang L M, Gao F, et al. Erythrocyte membrane is an alternative coating to polyethylene glycol for prolonging the circulation lifetime of gold nanocages for photothermal therapy. ACS Nano,2014, 8 (10): 10414–10425. DOI: 10.1021/nn503779d
[9]
Chen H C, Tian J W, He W J, et al. H2O2-activatable and O2-evolving nanoparticles for highly efficient and selective photodynamic therapy against hypoxic tumor cells. J. Am. Chem. Soc.,2015, 137 (4): 1539–1547. DOI: 10.1021/ja511420n
[10]
Weissleder R. A clearer vision for in vivo imaging. Nat. Biotechnol.,2001, 19 (4): 316–317. DOI: 10.1038/86684
[11]
Weissleder R, Ntziachristos V. Shedding light onto live molecular targets. Nat. Med.,2003, 9 (1): 123–128. DOI: 10.1038/nm0103-123
[12]
Ma Z Y, Yang M K, Foda M F, et al. Polarization of tumor-associated macrophages promoted by vitamin C-loaded liposomes for cancer immunotherapy. ACS Nano,2022, 26 (10): 17389–17401. DOI: 10.1021/acsnano.2c08446
[13]
Wu L, Fang S T, Shi S, et al. Hybrid polypeptide micelles loading indocyanine green for tumor imaging and photothermal effect study. Biomacromolecules,2013, 14 (9): 3027–3033. DOI: 10.1021/bm400839b
[14]
Zheng X H, Xing D, Zhou F F, et al. Indocyanine green-containing nanostructure as near infrared dual-functional targeting probes for optical imaging and photothermal therapy. Mol. Pharmaceut.,2011, 8 (2): 447–456. DOI: 10.1021/mp100301t
[15]
Yu J, Javier D, Yaseen M A, et al. Self-assembly synthesis, tumor cell targeting, and photothermal capabilities of antibody-coated indocyanine green nanocapsules. J. Am. Chem. Soc.,2010, 132 (6): 1929–1938. DOI: 10.1021/ja908139y
[16]
Yang H, Mao H J, Wan Z H, et al. Micelles assembled with carbocyanine dyes for theranostic near-infrared fluorescent cancer imaging and photothermal therapy. Biomaterials,2013, 34 (36): 9124–9133. DOI: 10.1016/j.biomaterials.2013.08.022
[17]
Wang Y, Yang T, Ke H T, et al. Smart albumin-biomineralized nanocomposites for multimodal imaging and photothermal tumor ablation. Adv. Mater.,2015, 27 (26): 3874–3882. DOI: 10.1002/adma.201500229
[18]
Han Y, Li J J, Zan M H, et al. Redox-responsive core cross-linked micelles based on cypate and cisplatin prodrugs-conjugated block copolymers for synergistic photothermal–chemotherapy of cancer. Polym. Chem.,2014, 5 (11): 3707–3718. DOI: 10.1039/C4PY00064A
[19]
Zheng M B, Yue C X, Ma Y F, et al. Single-step assembly of DOX/ICG loaded lipid–polymer nanoparticles for highly effective chemo-photothermal combination therapy. ACS Nano,2013, 7 (3): 2056–2067. DOI: 10.1021/nn400334y
[20]
Li Y L, Deng Y B, Tian X, et al. Multipronged design of light-triggered nanoparticles to overcome cisplatin resistance for efficient ablation of resistant tumor. ACS Nano,2015, 9 (10): 9626–9637. DOI: 10.1021/acsnano.5b05097
[21]
Bugaj J E, Achilefu S I, Dorshow R B, et al. Novel fluorescent contrast agents for optical imaging of in vivo tumors based on a receptor-targeted dye-peptide conjugate platform. J. Biomed. Opt.,2001, 6 (2): 122–133. DOI: 10.1117/1.1352748
[22]
Ye Y P, Bloch S, Kao J, et al. Multivalent carbocyanine molecular probes: Synthesis and applications. Bioconjugate Chem.,2005, 16 (1): 51–61. DOI: 10.1021/bc049790i
[23]
Bourré L, Thibaut S, Briffaud A, et al. Indirect detection of photosensitizer ex vivo. J. Photochem. Photobiol. B,2002, 67 (1): 23–31. DOI: 10.1016/S1011-1344(02)00279-8
[24]
Yuan Y, Min Y, Hu Q, et al. NIR photoregulated chemo- and photodynamic cancer therapy based on conjugated polyelectrolyte–drug conjugate encapsulated upconversion nanoparticles. Nanoscale,2014, 6 (19): 11259–11272. DOI: 10.1039/C4NR03302G
[25]
Knop K, Hoogenboom R, Fischer D, et al. Poly(ethylene glycol) in drug delivery: Pros and cons as well as potential alternatives. Angew. Chem. Int. Ed.,2010, 49 (36): 6288–6308. DOI: 10.1002/anie.200902672