Electric fields generated by synchronized oscillations of microtubules, centrosomes and chromosomes regulate the dynamics of mitosis and meiosis
© Zhao and Zhan; licensee BioMed Central Ltd. 2012
Received: 1 May 2012
Accepted: 26 June 2012
Published: 2 July 2012
Super-macromolecular complexes play many important roles in eukaryotic cells. Classical structural biological studies focus on their complicated molecular structures, physical interactions and biochemical modifications. Recent advances concerning intracellular electric fields generated by cell organelles and super-macromolecular complexes shed new light on the mechanisms that govern the dynamics of mitosis and meiosis. In this review we synthesize this knowledge to provide an integrated theoretical model of these cellular events. We suggest that the electric fields generated by synchronized oscillation of microtubules, centrosomes, and chromatin fibers facilitate several events during mitosis and meiosis, including centrosome trafficking, chromosome congression in mitosis and synapsis between homologous chromosomes in meiosis. These intracellular electric fields are generated under energy excitation through the synchronized electric oscillations of the dipolar structures of microtubules, centrosomes and chromosomes, three of the super-macromolecular complexes within an animal cell.
KeywordsPolar wind Chromosome Microtubule Centrosome Spindle body
The choreography of microtubules, centrosomes and chromosomes during mitosis and meiosis is beautifully designed by nature. Finely regulated and synchronized movements of these super-macromolecular complexes against the entropic forces within a dividing cell ensure the fidelity of the genetic material in both daughter cells. Currently, several models exist for the mechanisms of chromosome congression and spindle body assembly during M phase such as the search and capture model, kinetochore-mediated k-fibre formation, kinetochore motors contributing to congression, and the polar wind model. The mechanisms evoked by these models probably overlap, so there is redundancy among them, since mutations in the genes involved have only mild effects on chromosome congression during mitosis . Many open questions remain within these models. In the polar-wind model, an unknown force (also known as the ejection force) generated by the spindle poles is considered to push the chromosomes to the spindle equator. Laser microsurgery experiments show that chromosome fragments without kinetochores are invariably expelled from the spindle, and chromosomes without kinetochores can still move from the vicinity of the spindle pole to the spindle equator [1–3]. The ejection force of the spindle body is dependent on the polymerization of spindle body microtubules, as depolymerization of astral microtubules by nocodazole or colcemid prevents the expulsion of severed chromosome arms from the spindle, whereas stabilization of microtubules by taxol drives chromosomes to the periphery of the astral array . In addition, the driving force responsible for the pole-ward flux of spindle microtubules during metaphase remains uncharacterized .
Cellular electric fields have been studied in various cell types, and several studies have reported the existence of dielectrophoretic forces around cells [6–8]; electromagnetic interactions between cells have also been studied [9–11]. Cifra et al. proposed that microtubules, which comprise heterodimers polymerized into a helical structure, can generate an electric field under intracellular energy excitation [12–15]. Inhibition of microtubule polymerization by an external electromagnetic field has been reported by Kirson et al. [16, 17]. Pokorny´ et al. detected four peaks of electric field activity around yeast cells during M phase, which correlated with spindle body assembly, kinetochore microtubule capture, and mitotic spindle elongation during anaphase A and B, visualized by fluorescence microscopy . Comparing synchronized and unsynchronized tubulin mutants of yeast cells, Pokorny´ et al. verified that synchronized yeast cells show more electric activity during M phase than non-synchronized yeasts . Direct measurements of electric resonant oscillations in microtubules have been presented at conferences by A. Bandyopadhyay. The technical aspects of direct detection of electric fields within a living cell have been discussed in a recent review . Resonance absorption of external electromagnetic fields by cancers has been reported by Vedruccio et al. , and Zimmerman et al. reported that cancer cell proliferation is inhibited by specific modulation frequencies .
Coherent oscillations in microtubules can be explained by Fröhlich’s theory, which describes a system of oscillators with energy supply, linear and nonlinear coupling with a heat bath. If a sufficient energy supply is provided to this system, condensation of energy occurs in the lowest mode leading to its coherent excitation [23, 24]. Electrostatic but not electrodynamic interactions are screened over long distances (Debye Screening). Given an intracellular salt concentration of ~ 150 mM, the effectiveness of electrostatic interaction is shortened to the nanometer range (the Debye length is ~ 0.7-0.8 nm). However, resonant electrodynamic interactions, such as the electromagnetic interactions generated by electric oscillations within the cell, may play a role in the long-distance recruitment of biomolecules. Following Fröhlich, Preto et al. suggested that long-range electrodynamic interactions can be triggered only under resonance conditions, and such interactions are effective when one normal mode is statistically privileged, typically out of thermal equilibrium, which could be the case in the intracellular context [25, 26].
In this article, we integrate research from several disciplines to provide an ‘electric’ view of the dynamics of these super-macromolecular complexes in mitosis, meiosis and other relevant cellular events. From our theoretical point of view, many of the unidentified forces regulating major cellular dynamic events during mitosis are probably electric forces generated by the synchronized oscillation of the electric dipoles within these super-macro organelle structures. Chronic exposure to extremely low frequency electric fields could affect several key steps of mitosis and neuronal cell physiology, resulting in an increased risk for cancer.
The electrical properties of microtubules and centrosomes
Electric fields in centrosome separation and bipolar spindle body assembly
Mechanisms of centrosome separation and bipolar spindle body assembly have been discussed in a recent review . The process is still incompletely understood. Plus end-directed motor proteins such as kinesin 5 and minus end-directed motor proteins such as dynein are known to play dominant roles in centrosome separation and spindle assembly. However, centrosomal microtubules and microtubules of the nuclear envelope (NE) and cellular cortex need to move into close proximity for motor proteins to attach to both so they can generate the pulling forces. The current models assume a randomized mode of microtubule interaction, which is quite inefficient. For example, at a certain point a centrosome would have to stop moving until certain microtubules had grown sufficiently for appropriate bridging by motor proteins, particularly during prophase, when the centrosomes do not have many associated microtubules. When the electric fields of microtubules and centrosomes are considered, these structures are mutually attractive. Thus, centrosome movement along the microtubule networks of the cellular cortex and NE is more efficient. We can also envision a more autonomous mode of microtubule lattice formation within the cellular cortex and NE.
Electrical properties of duplicated chromosomes
Andrews et al. have studied the effects of high frequency (range 2 to 50 MHz) electric fields on mammalian (human and Chinese hamster) chromosomes in vitro. They showed that such chromosomes can be oriented, aligned and translated by an oscillating electrical force. They also observed that above certain threshold field strengths the chromosomes orient themselves with their long axes along the field direction. The dependence of this threshold on frequency was measured and was found to be much larger at low than at high frequencies . Using electric dichroism experiments, Crothers reported permanent dipole moments in dinucleosomes linked by 140 and 175 base pairs of DNA . Jian Sun et al. suggested an electrostatic mechanism of nucleosomal array folding, revealed by computer simulation, which explains the salt-dependent chromatin fiber conformations . Schalch et al. reported that the X-ray structure of an oligonucleosome revealed that linker DNA elements zigzag back and forth between two stacks of nucleosome cores, forming a truncated two-start helix, and do not follow a path compatible with a one-start solenoidal helix . Grigoryev et al. reported evidence for heteromorphic chromatin fibers, showing that the 2-start zigzag topology and the type of linker DNA bending that defines solenoid models may be simultaneously present in a structurally heteromorphic chromatin fiber with a uniform 30 nm diameter .
However, the physical mechanisms that regulate higher order packaging of M phase chromosomes are still not well characterized. Here we present a hypothesis of chromosome compaction. We apply a pulse-coupled oscillation clustering model to the dynamic events of chromosome packaging and inter-/intra-chromosomal organization. During chromosomal packaging, differentially compacted regions form partially synchronized electric oscillators interacting with an elastic electromagnetic field. According to the physical pulse-coupled oscillator model, unsynchronized pulse-coupled oscillators with proximal natural frequencies form synchronized oscillation clusters at a given coupling strength. As the coupling strength increases, these synchronized oscillation clusters merge with each other [37–40].
Theoretically, the oscillation clustering model explains the closely juxtaposed configuration of duplicated chromosomes during M phase, which is counter-intuitive from the perspective of electrostatic repulsion between duplicated chromosome arms. As the homologous chromosomal regions develop synchronized oscillation clusters with identical natural frequencies, they tend to cluster together. The same scenario could apply to synapsis during meiosis; the electric oscillations of homologous chromosomes couple with each other, preventing synapsis between non-homologous chromosomes.
Electric interactions during mitosis and meiosis
According to the physical organization of the duplicated chromosome arms, the condensed electric chromosomal fields around the centromeric regions could attract microtubule fragments to the sister kinetochores through electric interaction, which is consistent with observations of kinetochore movement along uncaptured microtubules, forming K-fibers (kinetochore associated microtubules) . Thus, electric interactions between chromosomes and microtubules may also facilitate K-fiber capture by kinetochores. The chromosome oscillation observed during congression could be explained as the turbulence of chromosome arms passing through the chaotic electric landscape of two astral microtubule networks.
In meiosis, the kinetochores are positioned at one side of the duplicated chromosome dimers, so the two sister chromosomes do not separate. The electric oscillation clustering between homologous chromosomal regions results in synapsis and recombination between homologous chromosomes; the electric fields generated by two duplicated homologous chromosomes can be viewed as two identical partially-entrained electric oscillation clusters, constituted by sub-chromosomal clusters throughout the chromosome arms. Such clusters in homologous chromosomes share identical electric frequencies, so the close juxtaposition between homologous chromosomes at synapsis is achieved through electric clustering and coupling among them. Synapsis does not occur during mitosis probably because the chromosome configuration caused by the opposing outward-pulling forces of the kinetochores at the opposite sides of duplicated centromere disfavors inter-chromosomal electric attraction. In addition, this event may be regulated by synaptonemal complex proteins .
Magidson et al. reported that chromosomes adopt a toroidal/ring shape organization of after NE breakdown, which facilitates spindle assembly during M phase . Their observation matches the electric model at several points: the ring shape organization could be generated by the electric interaction between M phase chromosomes and the spindle body, and the interplay between the electric fields of the chromosome ring and spindle body microtubules promotes the capture of microtubules by kinetochores.
Numerous reports indicate that extremely low frequency electric fields can increase the risks of certain types of cancer . Micronuclei (MN) in buccal mucosal cells, comprising acentric fragments or complete chromosomes that fail to attach to the mitotic spindle during cytokinesis, are increased in people chronically exposed to extremely low frequency electric fields . Research by Hardell et al. indicates increased brain tumor risks with latency time and cumulative mobile or cordless phone use . Volkow et al. reported that 50-minute cell phone exposure was associated with increased brain glucose metabolism in the region closest to the antenna . However, the exact cellular biophysical pathways that relay very low frequency electric radiations to genetic alterations that lead to cancer are not well characterized. From our theoretical point of view, chronic exposure to extremely low frequency electric fields would intervene in several key steps of mitosis and neuronal cell physiology, potentially resulting in an increased risk for cancer.
To characterize these intracellular electric fields and study their cellular functions further, biophysicists should develop more detailed mathematical and physical models for chromosome electric fields and their role in M phase chromosome compaction, to allow these fields to be described and calculated more precisely and to predict the dynamics of related cellular events. The dynamic of changes of the electric fields in a living cell during mitosis and other cellular processes could be visualized using live cell imaging technologies such as nano-sized voltmeters . It would be particularly interesting to observe microtubule self-organization under energy excitation in vitro, which would allow us to observe the dynamics of microtubule movements directly through electric interactions. These insights will help us to understand the molecular mechanisms of signal pathways better and to elucidate cellular super-macromolecular behavior, cell organelle organization and functions, intra- and inter-cellular communications, tissue morphogenesis, embryo development, neurobiology, and oncogenesis, and finally to advance our knowledge about life to a new level.
We thank Dr. Michal Cifra of Institute of Photonics and Electronics, Academy of Sciences of the Czech Republic and Dr. Yujie Sun of Biodynamic Optical Imaging Center of Peking University for their helpful discussion and insights about electric fields in live intracellular organelles. We thank Dr. Lennart Hardell of University Hospital, Sweden for providing us some of the latest epidemiological data linked with EMF and cancer. We also thank Editor-in-Chief of Theoretical Biology and Medical Modelling Dr. Paul Agutter for language editing of the article.
- Walczak CE, Cai S, Khodjakov A: Mechanisms of chromosome behavior during mitosis. Nat Rev Mol Cell Bio. 2009, 11: 91-102.Google Scholar
- Rieder CL, Davison EA, Jensen LCW, Cassimeris L, Salmon ED: Oscillatory movements of monooriented chromosomes and their position relative to the spindle pole result from the ejection properties of the aster and the half-spindle. J Cell Biol. 1986, 103: 581-591. 10.1083/jcb.103.2.581.View ArticlePubMedGoogle Scholar
- Khodjakov A, Rieder CL: Kinetochores moving away from their associated pole do not exert a significant pushing force on the chromosome. J Cell Biol. 1996, 135: 315-327. 10.1083/jcb.135.2.315.View ArticlePubMedGoogle Scholar
- Ault JG, DeMarco AJ, Salmon ED, Rieder CL: Studies on the ejection properties of asters: astral microtubule turnover influences the oscillatory behavior and positioning of mono-oriented chromosomes. J Cell Sci. 1991, 99: 701-710.PubMedGoogle Scholar
- Kwok BH, Kapoor TM: Microtubule flux: drivers wanted. Curr Opin Cell Biol. 2007, 19: 36-42. 10.1016/j.ceb.2006.12.003.View ArticlePubMedGoogle Scholar
- Pohl J, Christophers E: Photo inactivation and recovery in skin fibroblasts after formation of mono- and bifunctional adducts by furocoumarins-plus-UVA. J Invest Dermatol. 1980, 75 (4): 306-310. 10.1111/1523-1747.ep12530921.View ArticlePubMedGoogle Scholar
- Hölzel R, Lamprecht I: Electromagnetic fields around biological cells. Neural Net World. 1994, 4 (3): 327-Google Scholar
- Hölzel R: Electric Activity of Non-Excitable Biological Cells at Radio Frequencies. Electro- and Magnetobiol. 2001, 20: 1-View ArticleGoogle Scholar
- Albrecht-Buehler G: Surface extensions of 3 T3 cells towards distant infrared sources. J Cell Biol. 1991, 114: 493-502. 10.1083/jcb.114.3.493.View ArticlePubMedGoogle Scholar
- Albrecht-Buehler G: A rudimentary form of cellular vision. Proc Natl Acad Sci USA. 1992, 89: 8288-8292. 10.1073/pnas.89.17.8288.PubMed CentralView ArticlePubMedGoogle Scholar
- Albrecht-Buehler G: A Long-Range Attraction Between Aggregating 3T3 Cells Mediated By Near-Infrared Light Scattering. Proc Natl Acad Sci USA. 2005, 102 (14): 5050-5055. 10.1073/pnas.0407763102.PubMed CentralView ArticlePubMedGoogle Scholar
- Havelka D, Cifra M: Calculation of the electromagnetic field around microtubule. Acta Polytechnica Czech Technical University in Prague. CTU Publishing House. 2009, 49 (2–3): 58-63. ISSN 1210–2709Google Scholar
- Cifra M, Havelka D, Deriu MA: Electric Field Generated by Longitudinal Axial Microtubule Vibration Modes with High Spatial Resolution Microtubule Model. Electrodynamic Activity of Living Cells. J Physics: Conference Series. 2011, 329: 012013-Google Scholar
- Cifra M, Pokorný J, Havelka D, Kucera O: Electric field generated by axial longitudinal vibration modes of microtubule. Biosystems. 2010, 100 (2): 122-131. 10.1016/j.biosystems.2010.02.007.View ArticlePubMedGoogle Scholar
- Havelka D, Cifra M, Kučera O, Pokorný J, Vrba J: High-frequency electric field and radiation characteristics of cellular microtubule network. J Theor Biol. 2011, 286 (1): 31-40.View ArticlePubMedGoogle Scholar
- Kirson ED, Gurvich Z, Schneiderman R, Dekel E, Itzhaki A, Wasserman Y, Schatzberger R, Palti Y: Disruption of Cancer Cell Replication by Alternating Electric Fields. Cancer Res. 2004, 64: 3288-3295. 10.1158/0008-5472.CAN-04-0083.View ArticlePubMedGoogle Scholar
- Kirson ED, Dbalý V, Tovarys F, Vymazal J, Soustiel JF, Itzhaki A, Mordechovich D, Steinberg-Shapira S, Gurvich Z, Schneiderman R, Wasserman Y, Salzberg M, Ryffel B, Goldsher D, Dekel E, Palti Y: Alternating electric fields arrest cell proliferation in animal tumor models and human brain tumors. Proc Natl Acad Sci USA. 2007, 104 (24): 10152-10157. 10.1073/pnas.0702916104.PubMed CentralView ArticlePubMedGoogle Scholar
- Pokorny J, Hasek J, Jelınek F, Saroch J, Palan B: Electric activity of yeast cells in the M phase. Electro Magnetobiol. 2001, 20: 371-396.View ArticleGoogle Scholar
- Jelínek F, Cifra M, Pokorny J, Vanis J, Simsa J, Hasek J, Frydlová I: Measurement of Electrical Oscillations and Mechanical Vibrations of Yeast Cells Membrane Around 1kHz. Electric Biology and Medicine. 2009, 28 (2): 223-232. 10.1080/15368370802710807.View ArticleGoogle Scholar
- Kučera O, Cifra M, Pokorný J: Technical aspects of measurement of cellular electric activity. Eur Biophys J. 2010, 39 (10): 1465-1470. 10.1007/s00249-010-0597-8.View ArticlePubMedGoogle Scholar
- Vedruccio C, Meessen A: EM Cancer Detection by Means of Non Linear Resonance Interaction. 2004, Proceedings of PIERS 2004, Progress in Electromagnetics Research Simposium, Pisa, Italy, 909-912.Google Scholar
- Zimmerman JW, Pennison MJ, Brezovich I, Yi N, Yang CT, Ramaker R, Absher D, Myers RM, Kuster N, Costa FP, Barbault A, Pasche B: Cancer cell proliferation is inhibited by specific modulation frequencies. Br J Cancer. 2012, 106: 307-313. 10.1038/bjc.2011.523.PubMed CentralView ArticlePubMedGoogle Scholar
- Fröhlich H: Long-range coherence and energy storage in biological systems. International Journal of Quantum Chemistry. 1968, 2: 641-649. 10.1002/qua.560020505.View ArticleGoogle Scholar
- Fröhlich H: The biological effects of microwaves and related questions. Advances in Electronics and Electron Physics. 1980, 53: 85-152.View ArticleGoogle Scholar
- Preto J, Floriani E, Nardecchia I, Ferrier P, Pettini M: Experimental assessment of the contribution of electrodynamic interactions to long-distance recruitment of biomolecular partners, theoretical basis. Phys Rev E Stat Nonlin Soft Matter Phys. 2012, 85 (4–1): 041904-PMID 22680495View ArticlePubMedGoogle Scholar
- Preto J, Pettini M: Long-range resonant interactions in biological systems. arXiv. 120: 5187v1-Google Scholar
- Cairns RA, Harris IS, Mak TW: Regulation of cancer cell metabolism. Nat Rev Cancer. 2011, 11 (2): 85-95. 10.1038/nrc2981.View ArticlePubMedGoogle Scholar
- Pokorný J, Vedruccio C, Cifra M, Kučera O: Cancer physics: diagnostics based on damped cellular elastoelectrical vibrations in microtubules. Eur Biophys J. 2011, 40 (6): 747-759. 10.1007/s00249-011-0688-1.View ArticlePubMedGoogle Scholar
- Barbault A, Costa FP, Bottger B, Munden RF, Bomholt F, Kuster N, Pasche B: Amplitude-modulated electromagnetic fields for the treatment of cancer: discovery of tumor-specific frequencies and assessment of a novel therapeutic approach. J Exp Clin Cancer Res. 2009, 28 (1): 51-10.1186/1756-9966-28-51.PubMed CentralView ArticlePubMedGoogle Scholar
- Doxsey SJ: Re-evaluating centrosome function. Nature Rev Molec Biol. 2001, 2: 688-699. 10.1038/35089575.View ArticleGoogle Scholar
- Tanenbaum ME, Medema RH: Mechanisms of centrosome separation and bipolar spindle assembly. Dev Cell. 2010, 14, 19 (6): 797-806.View ArticleGoogle Scholar
- Andrews MJ, McClure JA: Effects of high frequency electric fields on mammalian chromosomes in vitro. J Biol Phys. 1979, 6 (1–2): 69-86. 10.1007/BF02311220.Google Scholar
- Crothers DM, Dattagupta N, Hogan M, Klevan L, Lee KS: Transient electric dichroism studies of nucleosomal particles. Biochemistry. 1978, 17 (21): 4525-4533. 10.1021/bi00614a026.View ArticlePubMedGoogle Scholar
- Sun J, Zhang Q, Schlick T: Electrostatic mechanism of nucleosomal array folding revealed by computer simulation. Proc Natl Acad Sci U S A. 2005, 102 (23): 8180-8185. 10.1073/pnas.0408867102.PubMed CentralView ArticlePubMedGoogle Scholar
- Schalch T, Duda S, Sargent DF, Richmond TJ: X-ray structure of a tetranucleosome and its implications for the chromatin fibre. Nature. 2005, 436: 138-141. 10.1038/nature03686.View ArticlePubMedGoogle Scholar
- Grigoryev SA, Arya G, Correll S, Woodcock CL, Schlick T: Evidence for heteromorphic chromatin fibers from analysis of nucleosome interactions. Proc Natl Acad Sci USA. 2009, 106 (32): 13317-13322. 10.1073/pnas.0903280106.PubMed CentralView ArticlePubMedGoogle Scholar
- Strogatz SH, Stewart I: Coupled oscillators and biological synchronization. Sci Am. 1993, 269 (6): 102-109. 10.1038/scientificamerican1293-102.View ArticlePubMedGoogle Scholar
- Morelli LG, Cerdeira H, Zanette DH: Frequency clustering of coupled phase oscillators on small-world networks. Eur Phys J B. 2005, 43: 243-250. 10.1140/epjb/e2005-00046-2.View ArticleGoogle Scholar
- Smet FD, Aeyels D: Clustering in a network of non-identical and mutually interacting agents. Proc R Soc A. 2009, 465: 745-768. 10.1098/rspa.2008.0259.View ArticleGoogle Scholar
- Aeyels D, Smet FD: Emergence and evolution of multiple clusters of attracting agents. Physica D. 2010, 239: 1026-1037. 10.1016/j.physd.2010.02.012.View ArticleGoogle Scholar
- Cifra M, Fields JZ, Farhadi A: Electromagnetic cellular interactions. Prog Biophys Mol Biol. 2011, 105 (3): 223-246. 10.1016/j.pbiomolbio.2010.07.003.View ArticlePubMedGoogle Scholar
- Olins DE, Olins AL: Chromatin history: our view from the bridge. Nat Rev Mol Cell Biol. 2003, 4: 809-814. 10.1038/nrm1225.View ArticlePubMedGoogle Scholar
- Annunziato A: DNA packaging: Nucleosomes and chromatin. Nature Education. 2008, 1 (1):Google Scholar
- Kollman JM, Merdes A, Mourey L, Agard DA: Microtubule nucleation by γ-tubulin complexes. Nat Rev Mol Cell Biol. 2011, 12: 709-721. 10.1038/nrm3209.View ArticlePubMedGoogle Scholar
- Rusan NM, Tulu US, Fagerstrom C, Wadsworth P: Reorganization of the microtubule array in prophase/prometaphase requires cytoplasmic dynein-dependent microtubule transport. J Cell Biol. 2002, 158: 997-1003. 10.1083/jcb.200204109.PubMed CentralView ArticlePubMedGoogle Scholar
- Tulu US, Rusan NM, Wadsworth P: Peripheral, non-centrosome-associated microtubules contribute to spindle formation in centrosome-containing cells. Curr Biol. 2003, 13: 1894-1899. 10.1016/j.cub.2003.10.002.View ArticlePubMedGoogle Scholar
- Magidson V, O'Connell CB, Lončarek J, Paul R, Mogilner A, Khodjakov A: The Spatial Arrangement of Chromosomes during Prometaphase Facilitates Spindle Assembly. Cell. 2011, 146 (4): 555-567. 10.1016/j.cell.2011.07.012. PMID: 21854981PubMed CentralView ArticlePubMedGoogle Scholar
- Petronczki M, Siomos MF, Nasmyth K: Un ménage à quatre: the molecular biology of chromosome segregation in meiosis. Cell. 2003, 112 (4): 423-40. 10.1016/S0092-8674(03)00083-7.View ArticlePubMedGoogle Scholar
- Baan R, Grosse Y, Lauby-Secretan B, El Ghissassi F, Bouvard V, Benbrahim-Tallaa L, Guha N, Islami F, Galichet L, Straif K, WHO International Agency for Research on Cancer Monograph Working Group: Carcinogenicity of radiofrequency electric fields. Lancet Oncol. 2011, 12 (7): 624-626. 10.1016/S1470-2045(11)70147-4.View ArticlePubMedGoogle Scholar
- Carbonari K, Gonçalves L, Roth D, Moreira P, Fernández R, Martino-Roth MG: Increased micronucleated cell frequency related to exposure to radiation emitted by computer cathode ray tube video display monitors. Genet Mol Biol. 2005, 28 (3): 469-474. 10.1590/S1415-47572005000300024.View ArticleGoogle Scholar
- Hardell L, Carlberg M, Mild KH: Pooled analysis of case–control studies on malignant brain tumours and the use of mobile and cordless phones including living and deceased subjects. Int J Oncol. 2011, 38 (5): 1465-1474. 10.3892.View ArticlePubMedGoogle Scholar
- Volkow ND, Tomasi D, Wang GJ, Vaska P, Fowler JS, Telang F, Alexoff D, Logan J, Wong C: Effects of Cell Phone Radiofrequency Signal Exposure on Brain Glucose Metabolism. JAMA. 2011, 305 (8): 808-813. 10.1001/jama.2011.186.PubMed CentralView ArticlePubMedGoogle Scholar
- Tyner KM, Kopelman R, Philbert MA: “Nanosized Voltmeter” Enables Cellular-Wide Electric Field Mapping. Biophys J. 2007, 93: 1163-1174. 10.1529/biophysj.106.092452.PubMed CentralView ArticlePubMedGoogle Scholar
This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.