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J.S. Abramowicz
30. Stewart HF, Stratmeyer ME. An overview of ultra­sound theory, measurement, medical applications and biological effects. US Department of Health and Human Services Publications; FDA 82-8190, US Government Printing Offi ce: 1982.
31. Thomenius KE, Lewin PA. Ultrasound bioeffects
1991. Ultrasound Q. 1991;9:111–37.
32. Dickey RP. Doppler ultrasound investigation of uter­ine and ovarian blood fl ow in infertility and early pregnancy. Hum Reprod Update. 1997;3:467–503.
33. Engels V, Sanfrutos L, Perez-Medina T, et al. Periovulatory follicular volume and vascularization determined by 3D and power Doppler sonography as pregnancy predictors in intrauterine insemination cycles. J Clin Ultrasound. 2011;39:243–7.
34. Sheiner E, Hackmon R, Shoham-Vardi I, et al. A com­parison between acoustic output indices in 2D and 3D/4D ultrasound in obstetrics. Ultrasound Obstet Gynecol. 2007;29:326–8.
35. Marsal K. The output display standard: has it missed its target? Ultrasound Obstet Gynecol. 2005;25: 211–4.
36. Sheiner E, Abramowicz JS. Clinical end users world­wide show poor knowledge regarding safety issues of ultrasound during pregnancy. J Ultrasound Med. 2008;27:499–501.
37. Akhtar W, Arain MA, Ali A, et al. Ultrasound bio­safety during pregnancy: what do operators know in the developing world?: national survey fi ndings from Pakistan. J Ultrasound Med. 2011;30:981–5.
38. Sharon N, Shoham-Vardi I, Aricha-Tamir B, Abramowicz JS, Sheiner E. [What do ultrasound per­formers in Israel know regarding safety of ultrasound, in comparison to the end users in the United States?]. Harefuah. 2012;151:146–9, 90.
39. Bagley J, Thomas K, DiGiacinto D. Safety practices of sonographers and their knowledge of the biologic effects of sonography. J Diagn Med Sonography. 2011;27:252–61.
40. Houston LE, Allsworth J, Macones GA. Ultrasound is safe… right?: resident and maternal-fetal medicine fellow knowledge regarding obstetric ultrasound safety. J Ultrasound Med. 2011;30:21–7.
41. Nyborg WL. History of the American Institute of Ultrasound in Medicine’s efforts to keep ultrasound safe. J Ultrasound Med. 2003;22:1293–300.
42. Karagoz I, Kartal MK. A new safety parameter for diagnostic ultrasound thermal bioeffects: safe use time. J Acoust Soc Am. 2009;125:3601–10.
43. Ziskin MC. The thermal dose index. J Ultrasound Med. 2010;29:1475–9.
44. Bigelow TA, Church CC, Sandstrom K, et al. The ther­mal index: its strengths, weaknesses, and proposed improvements. J Ultrasound Med. 2011;30:714–34.
45. Queenan JT, O’Brien GD, Bains LM, Simpson J, Collins WP, Campbell S. Ultrasound scanning of ova­ries to detect ovulation in women. Fertil Steril. 1980;34:99–105.
46. Vesper B, Schulte HR. [Ultrasonic follow-up check of overstimulation by gonadotrophin therapy (author’s transl)]. Zentralbl Gynakol. 1980;102:791–6.
47. Lenz S, Lauritsen JG, Kjellow M. Collection of human oocytes for in vitro fertilisation by ultrasonically guided follicular puncture. Lancet. 1981;1:1163–4.
48. Renaud R, Ehret C, Dervain I, Plas-Roser S, Aron C, Spira A. [Ovarian sonography: a new way of monitor­ing ovulation induction treatments]. Bull Acad Natl Med. 1981;165:353–8.
49. Bologne R, Demoulin A, Schaaps JP, Hustin J, Lambotte R. [Infl uence of ultrasonics on the fecundity of female rats]. C R Seances Soc Biol Fil. 1983;177: 381–7.
50. Demoulin A, Bologne R, Hustin J, Lambotte R. Is ultrasound monitoring of follicular growth harmless? Ann N Y Acad Sci. 1985;442:146–52.
51. Quereux C, Mazili ML, Desroches A, et al. Does ultrasound have an adverse effect on the fertility of women? J Gynecol Obstet Biol Reprod (Paris). 1986;15:159–64.
52. Feichtinger W, Putz M, Kemeter P. [Transvaginal Doppler sonography for measuring blood fl ow in the pelvis]. Ultraschall Med. 1988;9:30–6.
53. Deutinger J, Reinthaller A, Bernaschek G. Transvaginal pulsed Doppler measurement of blood fl ow velocity in the ovarian arteries during cycle stim­ulation and after follicle puncture. Fertil Steril. 1989;51:466–70.
54. Fleischer AC. Ultrasound imaging–2000: assessment of utero-ovarian blood fl ow with transvaginal color Doppler sonography; potential clinical applications in infertility. Fertil Steril. 1991;55:684–91.
55. Campbell S, Bourne TH, Waterstone J, et al. Transvaginal color blood fl ow imaging of the periovu­latory follicle. Fertil Steril. 1993;60:433–8.
56. Abramowicz JS, Jaffe R, Pierson R. Transvaginal color Doppler assessment of uterine and ovarian blood fl ow during normal and abnormal cycles. In: Jaffe R, Pierson R, Abramowicz JS, editors. Imaging in infertility and reproductive endocrinology. Philadelphia: J.B. Lippincott; 1994.
57. Altundag M, Levi R, Adakan S, et al. Intraovarian stromal artery Doppler indices in predicting ovarian response. J Reprod Med. 2002;47:886–90.
58. Jarvela IY, Sladkevicius P, Kelly S, Ojha K, Campbell S, Nargund G. Quantifi cation of ovarian power Doppler signal with three-dimensional ultrasonogra­phy to predict response during in vitro fertilization. Obstet Gynecol. 2003;102:816–22.
59. Merce LT, Gomez B, Engels V, Bau S, Bajo JM. Intraobserver and interobserver reproducibility of ovarian volume, antral follicle count, and vascularity indices obtained with transvaginal 3-dimensional ultrasonography, power Doppler angiography, and the virtual organ computer-aided analysis imaging pro­gram. J Ultrasound Med. 2005;24:1279–87.
60. Marret H, Brewer M, Giraudeau B, Tranquart F, Voelker K, Satterfi eld W. Ovine model to evaluate ovarian vascularization by using contrast-enhanced sonography. Comp Med. 2005;55:150–5.
61. Marret H, Brewer M, Giraudeau B, Tranquart F, Satterfi eld W. Assessment of cyclic changes of
1 Ultrasound in Reproductive Medicine: Is It Safe?
15
microvessels in ovine ovaries using Sonovue contrast­enhanced ultrasound. Ultrasound Med Biol. 2006;32:163–9.
62. Duck FA, Starritt HC, ter Haar GR, Lunt MJ. Surface heating of diagnostic ultrasound transducers. Br J Radiol. 1989;62:1005–13.
63. Gleicher N, Friberg J, Fullan N, et al. EGG retrieval for in vitro fertilisation by sonographically controlled vaginal culdocentesis. Lancet. 1983;2:508–9.
64. Heyner S, Abraham V, Wikarczuk ML, Ziskin MC. Effects of ultrasound on ovulation in the mouse. Gamete Res. 1989;22:333–8.
65. Heyner S, Abraham V, Wikarczuk ML, Ziskin MC. Effects of ultrasound on DNA and RNA synthesis in preimplantation mouse embryos. Mol Reprod Dev. 1990;25:209–14.
66. Mahadevan M, Chalder K, Wiseman D, Leader A, Taylor PJ. Evidence for an absence of deleterious effects of ultrasound on human oocytes. J In Vitro Fert Embryo Transf. 1987;4:277–80.
67. Williams SR, Rothchild I, Wesolowski D, Austin C, Speroff L. Does exposure of preovulatory oocytes to ultrasonic radiation affect reproductive performance? J In Vitro Fert Embryo Transf. 1988;5:18–21.
68. Kerin JF. Determination of the optimal timing of insemination in women. In: Richardson D, Joyce D, Symonds M, editors. Frozen human semen. London: Royal College of Obstetrics and Gynaecology; 1979. p. 105–32.
69. Brent RL, Beckman DA, Landel CP. Clinical teratol­ogy. Curr Opin Pediatr. 1993;5:201–11.
70. Takeuchi H, Nakazawa T, Kumakiri K, Kusano R. Experimental studies on ultrasonic Doppler method in obstetrics. Acta Obstet Gynaecol Jpn. 1970;17:11–6.
71. Stolzenberg SJ, Torbit CA, Edmonds PD, Taenzer JC. Effects of ultrasound on the mouse exposed at differ­ent stages of gestation: acute studies. Radiat Environ Biophys. 1980;17:245–70.
72. Stolzenberg SJ, Edmonds PD, Torbit CA, Sasmore DP. Toxic effects of ultrasound in mice: damage to central and autonomic nervous systems. Toxicol Appl Pharmacol. 1980;53:432–8.
73. Brodal P. Restitution of function after brain damage. In: Brodal P, editor. The central nervous system Structure and function. 4th ed. New York: Oxford University Press; 2010. p. 147–56.
74. Edwards MJ, Saunders RD, Shiota K. Effects of heat on embryos and foetuses. Int J Hyperthermia. 2003;19:295–324.
75. Ang ESBC, Gluncic V, Duque A, Schafer ME, Rakic P. Prenatal exposure to ultrasound waves impacts neu­ronal migration in mice. Proc Natl Acad Sci U S A. 2006;103:12903–10.
76. Graham Jr JM, Edwards MJ, Edwards MJ. Teratogen update: gestational effects of maternal hyperthermia due to febrile illnesses and resultant patterns of defects in humans. Teratology. 1998;58:209–21.
77. Stalberg K, Haglund B, Axelsson O, Cnattingius S, Pfeifer S, Kieler H. Prenatal ultrasound and the risk of childhood brain tumour and its subtypes. Br J Cancer. 2008;98:1285–7.
78. Calvert J, Duck F, Clift S, Azaime H. Surface heating by transvaginal transducers. Ultrasound Obstet Gynecol. 2007;29:427–32.
79. McClain RM, Hoar RM, Saltzman MB. Teratologic study of rats exposed to ultrasound. Am J Obstet Gynecol. 1972;114:39–42.
80. Sikov MR, Hildebrand BP. Embryotoxicity of ultra­sound exposure at nine days of gestation in the rat. In: White D, Braun RE, editors. Ultrasound in medicine. New York: Plenum Press; 1977.
81. Sikov MR, Hildebrand BP. Effects of ultrasound on the prenatal development of the rat. Part 1. 3.2 MHz continuous wave at nine days of gestation. J Clin Ultrasound. 1976;4:357–63.
82. Schneider-Kolsky ME, Ayobi Z, Lombardo P, Brown D, Kedang B, Gibbs ME. Ultrasound exposure of the foetal chick brain: effects on learning and memory. Int J Dev Neurosci. 2009;27:677–83.
83. Hussain R, Kimme-Smith C, Tessler FN, Perrella RR, Grant EG, Sandstrom K. Fetal exposure from endo­vaginal ultrasound examinations in the fi rst trimester. Ultrasound Med Biol. 1992;18:675–9.
84. Miller MW, Ziskin MC. Biological consequences of hyperthermia. Ultrasound Med Biol. 1989;15: 707–22.
85. Zhang J, Zhou F, Song Y, Ying W, Zhang Y. Long dwell-time exposure of human chorionic villi to trans­vaginal ultrasound in the fi rst trimester of pregnancy induces activation of caspase-3 and cytochrome C release. Biol Reprod. 2002;67:580–3.
86. Abramowicz JS, Fowlkes JB, Skelly AC, Stratmeyer ME, Ziskin MC. Conclusions regarding epidemiology for obstetric ultrasound. J Ultrasound Med. 2008;27: 637–44.
87. Sheiner E, Shoham-Vardi I, Pombar X, Hussey MJ, Strassner HT, Abramowicz JS. An increased thermal index can be achieved when performing Doppler stud­ies in obstetric sonography. J Ultrasound Med. 2007; 26:71–6.
88. AIUM. AIUM practice guideline for the performance of obstetric ultrasound examination. J Ultrasound Med. 2010;29:157–66.
89. Miller MW, Brayman AA, Abramowicz JS. Obstetric ultrasonography: a biophysical consideration of patient safety–the “rules” have changed. Am J Obstet Gynecol. 1998;179:241–54.
90. Duck FA. Is it safe to use diagnostic ultrasound during the fi rst trimester? Ultrasound Obstet Gynecol. 1999;13:385–8.
91. Nelson TR, Fowlkes JB, Abramowicz JS, Church CC. Ultrasound biosafety considerations for the practicing sonographer and sonologist. J Ultrasound Med. 2009;28:139–50.
92. Safety Group of the British Medical Ultrasound Society (BMUS). Guidelines for the safe use of diag­nostic ultrasound equipment. Ultrasound. 2010;18: 52–9.
93. Abramowicz JS. Fetal Doppler: how to keep it safe?
Clin Obstet Gynecol. 2010;53:842–50.
94. Abramowicz JS, Sheiner E. Ultrasound bioeffects
and safety: what the practitioner should know. In:
16
J.S. Abramowicz
Fleischer AC, Manning FA, Jeanty P, Romero R, edi­tors. Sonography in obstetrics and gynecology- principles and practice. 7th ed. New York: McGraw-Hill; 2010.
95. AIUM. AIUM Offi cial Statement. Statement on the safe use of Doppler ultrasound during 11-14 week scans (or earlier in pregnancy); 2011.
org/offi cialstatements/42
96. AIUM. AIUM Offi cial Statement. Prudent use in preg­nancy; 2012. Accessed on March 2013.
97. AIUM. AIUM As Low As Reasonably Achievable (ALARA) principle; 2012.
statements/39
. Accessed on March 2013.
. Accessed on March 2013.
http://aium.org/offi cialstatements/33 .
http://aium.org/offi cial-
http://aium.
98. Ter Haar G. Ultrasound imaging: safety consideration. Interface Focus. 2011;1(14):686–97. doi:
rsfs.2011.0029
99. Chervenak FA, McCullough LB. Research on the fetus using Doppler ultrasound in the fi rst trimester: guiding ethical considerations. Ultrasound Obstet Gynecol. 1999;14:161.
100. Campbell S, Platt L. The publishing of papers on fi rst-trimester Doppler. Ultrasound Obstet Gynecol. 1999;14:159–60.
. Epub 2011 May 25.
10.1098/

Principles of 3D Ultrasound

Maximilian Murtinger , Dietmar Spitzer , and Nicolas Herbert Zech
2

Introduction

Ultrasound (US) performance is a noninvasive, painless procedure. Its applications are essential for IVF (in vitro fertilization) therapy; employed US frequencies range between 1 and 18 MHz, which have no known harmful effects to the patients, their gametes, or embryos [ 1 , 2 ].
Two-dimensional ultrasound (2D US) has been used in medical applications for decades, notably in artifi cial reproduction technology (ART). Interestingly, the fi rst commercial three­dimensional visualization was achieved not by US but by magnetic resonance imaging (MRI) and computed tomography (CT). However, the fi rst reports on 3D US appeared in the early 1980s, almost simultaneously with the appear­ance of CT and MRI [ suffered from several initial problems. As a result, more than one decade passed before the fi rst commercial 3D US became available and
M. Murtinger , MD IVF Centers Prof. Zech, Römerstrasse 2, Bregenz 6900, Austria e-mail: m.murtinger@ivf.at
N. H. Zech , MD (*) Department of Obstetrics and Gynecology, Medical University Graz, Römerstrasse 2, 6900 Bregenz , Austria e-mail: n.zech@ivf.at
D. Spitzer , MD IVF Centers Prof. Zech, Innsbrucker Bundesstrasse 35, Salzburg 5000, Austria e-mail: d.spitzer@salzburg.ivf.at
3 – 5 ]. Nevertheless, 3D US
was introduced for clinical applications. This was due to several factors. First, the development of 3D US imaging had been limited by comput­ing power, which, until the last decade, restricted 3D reconstruction to offl ine work stations. Second, the clinical approach was handicapped by problems intrinsic to US imaging: speckle, clutter, grating lobe, and other artifacts [ Additionally, in the past the storage of 3D images was unfeasible due to the limited storage capac­ity of the computers as well as the post-process­ing procedures, which are now considerably facilitated by highly effi cient hardware and soft­ware. With the new data processors, the recon­struction procedure of 2D scans into 3D structures can be carried out within a few sec­onds after the images have been acquired. Three­dimensional images can also be generated with 2D ultrasound computed tomography, either by shifting the measurement arrangement or by moving the analyzed object. By this approach, at each step only one layer is recorded, which is then composed to a full-dimensional structure. Therefore, even with conventional US scanners, a composited 3D imaging (spatial compounding) can be generated. Important for this technique is the matching of the set of 2D images. The 3D images are calculated by combining the informa­tion on the position and angulation of the images. The required positional information is obtained either by the conventional probe, the position of the transducer measured, or by using a special scanner. However, a system for positioning and orientation of the scanner is still needed. To
6 ].
L.A. Stadtmauer, I. Tur-Kaspa (eds.), Ultrasound Imaging in Reproductive Medicine, DOI 10.1007/978-1-4614-9182-8_2, © Springer Science+Business Media New York 2014
17
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M. Murtinger et al.
reduce the number of orientations, special types of ultrasound transducer systems were devel­oped, allowing the acquisition of information through only one viewing direction by electronic focusing.
In 1984, Kazunori Baba fi rst described a 3D ultrasound system. In 1986, he was the fi rst per­son on the globe to obtain 3D images of a 19-week fetus by processing the raw 2D images on a minicomputer in 1986 [ 7 , 8 ]. In 1987 Olaf T. von Ramm and Steven W. Smith patented “An acoustic pulse echo imaging system capable of producing an image of a three-dimensional object utilizing a two-dimensional display. In the system angular relationships of targets at all ranges are maintained for display. The system uses a two- dimensional transducer array of piezoelectric elements; the array is steered to assume transmit and receive orientations in both azimuth and elevation by producing (1) a directed transmit pulse and many similarly directed receive orientations or (2) a non-directed transmit pulse and many directed receive orien­tations. For each transmit pulse a parallel pro­cessing system produces several unique image points whose locations in the image correspond to the tangents of the angles of the receive orien­tations in the azimuth and elevation planes. The brightness of each image point is the weighted integral of the echo data received along each receive path. As an option, range discrimination capability is provided by means of a range dependent gain control, brightness shading as a function of range or a color display in which data originating from different ranges is displayed in different hues [ 9 ].”
Two years later, the fi rst commercially avail­able 3D US instrument was marketed in 1989 by the Austrian company Kretztechnik (Zipf/ Austria) which was founded by the engineer Paul Kretz after the Second World War.
This instrument, the Combison 330 equipped with 7.5 MHz and integrated 3D system was pre­sented at the French radiology congress in Paris in 1989 [ 10 ]. It utilized mechanical abdominal volume scan transducers with the mechanical swept-volume approach. Although the acquisi­tion of the volume took only 1–2 s, rendering of the image took up to almost 20 min on an exter-
nal computer. However, the rendering was also limited in ability to provide a set of orthogonal planes orientated images in strict relation to the axis of the probe. Additionally, special scan transducers were needed for this instrument. They had to be held by their larger side, thus making them rather diffi cult to handle. This drawback was removed in the majority of the later US instruments by a 90° rotation of the 3D US device. In 1998, the Voluson 530D 3D system implemented a technology that displayed not only the 3D sectional images, but also processed the data of the entire volume in real time. With the commercial launch of this 3D instrument platform, 3D ultrasound technology competed with the higher priced CT and MRI instruments; it allowed effective grayscale imaging, spectral Doppler, color Doppler, and Angio Color Imaging [ 11 ]. Two years later, the medical equipment manufacturer GE Healthcare introduced a new generation of clinical US systems, the Voluson 730 with real-time acquisition of volumes (16 volumes/s). Now, it is possible to detect and ana­lyze even moving objects such as a fetus. With the beginning of the new millennium, several new software programs became available that signifi cantly improved the image quality.
Currently, numerous 3D US instruments are available (most of them semi- or fully auto­mated), and it is extremely likely that dozens of new machines will become available in the next few years. The systems have become faster and more advanced. Furthermore, the number of compatible software programs exceeds the amount of instruments sold. Virtual naviga­tion, different modes of presentation (such as tomographic ultrasound imaging (TUI) volume, contrast imaging (VCI) and automated volume calculation (SonoAVC), computer-aided analy­sis (VOCAL) calculation) , and other techniques are now available; they are reliable, fast, and user friendly [ 12 ]. With these features, the pos- sibilities for clinical application become almost unlimited; furthermore, use is increasing in the clinical setting. Many post-processing tools such as speckle reduction imaging, electronic scalpel, and fi lters for brightness and contrast facilitate handling. Data transfer and long-term storage are now possible without any quality
2 Principles of 3D Ultrasound
19
loss. Although most procedures are still con­ducted with 2D scans, for a number of rea­sons, it is likely that the 3D technology will be a supplementary tool—and in some cases, a replacement—for 2D instruments in the fi eld of ART in the future.

Basic Techniques of 3D US

The basic techniques of 3D US systems are almost identical to those of 2D systems because they use the same frequencies and wavelengths. According to the US Food and Drug Administration (FDA), the limit for obstetrical ultrasound is 94 mW/cm 2 for the spatial peak temporal average intensity and 190 W/cm 2 for spatial peak pulse average for fetal imaging [ 13 ]. The principles of 3D Doppler US technology are not a subject of this chapter but are summarized in detail in a previous chapter.
Three-dimensional sonography in medicine comprises data acquisition, analysis and process­ing of volume, image animation and fi nalizing of the image, and data storage [ 14 ]. In principle, there are three (respectively four) ways of achiev­ing 3D data:
1. The tracked freehand method: Freehand 3D
ultrasound allows intraoperative imaging of
volumes of interest in a rapid and fl exible
manner [ 15 ]. This technique requires manual
movement of the probe through the ROI
(region of interest). However, as a prerequi-
site the exact angulation and position of the
US transducer are needed.
2. The untracked freehand systems: With these
systems, the operator moves the transducer in
a regular motion, while the 2D images are per-
formed. For a 3D image a linear or angular
spacing between the single images is assumed.
The major disadvantage of this technique is
that exact local positioning is not possible and
measurements, especially for volumes, are
highly inaccurate.
3. A three-dimensional visualization can be
intrinsically achieved by 2D transducer
arrays: These arrays generate pyramidal
pulses of the US and the echoes are converted
into 3D images. The advantage is that the
transducer can remain stationary and elec­tronic scanning can be used to sweep a broad ultrasound beam over the entire volume under examination [ 16 ].
4. A fourth possibility is mechanical assemblies: The transducer is moved either (1) linear, (2) tilted, or (3) in a rotational movement about its central axis by a mechanical assembly.

Reconstruction and Visualization of 3D Images and Post-processing

Software programs for reconstruction (render­ing) and imaging play a dominant role in 3D US. Several algorithms have been developed allow­ing for perfect visualization, manipulation, and processing of the received 3D images. It is appar­ent that the progress in software development was—and still is—the key to success for this technique. Currently, numerous visualization modalities are available:
1. Multi-planar view: This was the fi rst available visualization mode in 3D US. The display pres­ents the three orthogonal planes simultane­ously: the longitudinal, transverse, and coronal planes. The dataset can then be rotated or sliced in order to view the region of interest (ROI). The multi-planar view displays the exact spa­tial relationships between the three planes.
2. The tomographic ultrasound imaging (TUI) or multi-slice technique: TUI allows for a com­prehensive sequential analysis of the desired organ (Fig. 2.1 ). The same imaging principle is employed in CT and MRI. For example, tomographic ultrasound imaging has been reported to greatly simplify pelvic fl oor assessment [ 17 ].
3. The static volume contrast imaging (VCI)
mode: This mode allows for the receipt of information from adjacent slices in a volume. This imaging mode was especially developed to enhance the contrast between tissues or organs that would appear similar on conven­tional 2D US [ 18 ]. VCI is currently applied for detecting thoracic abnormalities [ 18 ] or imaging fetal pelvic anatomy [ 19 ]; it was found to be superior to 2D US in these studies.
20
Fig. 2.1 Tomographic ultrasound image (TUI) of multiple follicles in a stimulated ovary
M. Murtinger et al.
4. Inversion mode: In inversion mode, volumes are displayed in their entirety as an echogenic area, while the grayscale portions of the image are rendered as transparent. Some IVF and obstetrical applications could benefi t from this method [ 20 ].
5. Transparency mode: The transparency mode (also known as maximum mode) images regions with high echo density in a glass-like mode. This mode is mostly used for imaging of cartilaginous structures. With this mode, high-echogenic voxels are higher valued.
6. The surface-rendering mode helps to detect and display the surface of the structures. It is most commonly used for the evaluation of ovarian tumors [ 21 , 22 ]. This technique allows surface reconstruction of conspicuous parietal structures [ 21 ].
7. Glass-body rendering: Glass-body rendering (GBR) imaging is a combination of the trans­parency and color or power Doppler mode. It is very suitable for gynecologic applications; however, it is most useful for vessel imaging. In this mode the rendering algorithm is based on the simultaneous representation of gray and color Doppler scale [ 23 ].
8. Four-dimensional image techniques: The four-dimensional image techniques (such as the spatiotemporal image correlation (STIC)) allow for procedures such as echocardiogra­phy of the fetal heart [ 24 , 25 ]. The received data is acquired by a single, automatic volume sweep; subsequently, the software analyzes the data according to their spatial and tempo­ral domain and processes a 4D cine sequence. Prior to the launch of these 4D techniques, the examination of the fetal heart with conven­tional US was often diffi cult.
9. OmniView: OmniView (GE Medical Systems, Kretztechnik, Zipf, Austria) is a recently developed display technology for 3D and 4D US that allows integration of volume datasets and the simultaneous display of up to three independent (non-orthogonal) planes by manually drawing straight or curved lines from any direction or angle [ 26 ].
Although many 3D US display techniques have been employed (more than the ones described in this chapter), the two most com­monly used are multi-planar reformatting and volume contrast rendering. Image quality has improved since the 1990s; nevertheless,
2 Principles of 3D Ultrasound
21
the fi nal quality still depends on the accu­racy of the scanned volumes (also see next paragraph). Nevertheless, as previously men­tioned, various software-based tools are cur­rently available. Post-processing is done via the electronic scalpel (Kretztechnik, Zipf, Austria), contrast and brightness regulation, or speckle reduction imaging (SRI). SRI was established on the Voluson platform in 2004 by GE Healthcare. The electronic scalpel allows for the removal of pre-located obscur­ing structures in three steps: (1) rotation of the rendered image into a position where the obscuring structures can be cut; (2) the selec­tion of the cutting mode; and (3) creation of the outline for the cut and activation of the cutting mode [ 27 ]. Speckles are recurrent problems in sonography due to interference of ultrasound echoes; they produce diffi cul­ties in differentiating anatomical structure. Many approaches have been attempted with the goal of reducing or even of eliminating speckles. Most signifi cantly, the increased computer processing power and speed of calculation within recent years have allowed more complex image-processing techniques to reduce these artifacts without impair­ing image quality [ 28 ]. In addition, fi lter- ing is widely used for undesired echoes that are a recurrent phenomenon in sonography. Filtering allows the suppression of unwanted background noise or the enhancement of the desired information (suppressing and enhanc­ing fi lters) [ 29 ] .
Initially, data storage was a problem with 3D technology. This problem has been resolved by the improved storage capacity of the hard disk. The acquired data can be readily stored without quality loss either at the US systems itself or on external media (CD, DVD, USB, or external hard drive). The data can still be post-processed with medical software and can be transferred, for example, via (virtual private network) VPN tunneling to another physician. Most importantly, the data can be reloaded and subjected to an additional expert opinion or used for education [ 30 ]. This is an invaluable feature. Currently, this capability facilitates optimal patient care.
Moreover, it might reduce medical malpractice and might prove to be an essential step towards standardization in this fi eld.

Advantages and Shortcomings of 3D US Techniques

Three-dimensional US allows visualization of all three image planes (sagittal, transverse, and cor­onal) of the analyzed object, including planes not accessible by 2D US. The viewed planes can be chosen or changed by the user to view the desired region under investigation. Using the conventional 2D technique, the referring physi­cian often had to integrate all the received 2D images in a three-dimensional form to obtain an impression about the anatomy and possible pathologies.
The use of 2D ultrasound for measurement of organs, such as the uterus or follicle volume, is variable and at times inaccurate. Some diagnostic and treatment IVF procedures require accurate volume measurements (such as follicle monitor­ing). The accurate acquisition of volumes is only possible with 3D US, especially when the ana­lyzed structures are not spherical but complex (i.e., follicles within a multi-follicular growth complex; this problem will be discussed in a subsequent chapter). 3D US is a relatively new technique for gynecology and IVF. However, studies have already been published reporting high accuracy.
Use of the 3D technique together with the appropriate software allows for the accessed 3D volumes to be digitally stored. This is a tremen­dous advantage for later post-processing and evaluation. Thus, the stored data can be reformat­ted and analyzed in various ways. Beyond all the technical improvements, 3D US is still based on conventionally received 2D US data. Thus, poor US scanning techniques cannot be improved by this innovative technique. Inadequate resolution of 2D scans results in poor image quality of the three- dimensional structures. Therefore the 2D scans must be optimized in regard to (1) bright­ness, (2) the depth of fi eld, and (3) the correct positioning of focus. The correct setting to
22
M. Murtinger et al.
achieve the optimal 2D scan is therefore a prereq­uisite for the best possible 3D calculation.
In addition, most artifacts, which are common in 3D or 4D US, are also similar to those of 2D US because both techniques are based on the same principle. Improper calibration and opera­tion is one major source of the production of infe­rior data as well as for poor interobserver reliability. This holds true for both, 2D and 3D US. One exception might be the appearance of artifacts due to the movement of the examined objects with 4D US. However, the application of 4D US does not play a dominant role in ART because most of the analyzed structures are immotile. However, it is not unequivocally clear whether the 4D technique might be of future value for ART. For example, endometrial blood fl ow analyzed by 4D US might become an addi­tional parameter for the prediction of embryo implantation in the future.
The 3D visualization technique offers no additional advantages in regard of reducing the aforementioned artifacts. The effective improve­ments of US imaging is due to accompanying post- processing software. However, this techni­cal processing cannot be regarded separately as these are integrated components of high-quality 3D instruments.
The rapidly increasing processing power was also one basic requirement for the introduction of portable US systems. This innovation, together with standardized higher image quality, standard­ized image storage, and compression techniques such as the Digital Imaging and Communications in Medicine (DICOM) standard, enables a medi­cal network and improved patient care.

Applications of 3D Ultrasound in ART

Several clinical trials have demonstrated the superiority of 3D systems compared to conven­tional 2D US. The images of the structure’s sur­faces become fully apparent (as a result of their three-dimensional nature). The detailed advan­tages of the 3D sonography, especially for IVF, are discussed within the Chap. 20 . However,
studies concerning 3D US in the context of IVF therapies are still limited. Conversely, 3D US in monitoring is commonly used during pregnancy and a crucial tool in prenatal diagnosis because the volumes of fetal organs can be accessed more accurately by the new 3D techniques rather than by conventional 2D US. Thus, fetal anomalies can be recognized more readily [ 31 , 32 ].
The applications of 3D US in IVF are also summarized in the Chap. 20 . However, an over- view of the applications of 3D sonography will be presented here. The investigation of the uterus, ovaries, and fallopian tubes are a prerequisite of an IVF cycle. Uterine pathology such as myo­mas, malformations (see Figs. 2.2 and 2.3 ) and carcinomas can signifi cantly impair the outcome of IVF therapy [ 33 ], and sometimes patient health. In addition to MRI and CT, 2D US was and is currently used for the detection of congeni­tal malformations of the female reproductive sys­tem. However, it lacks specifi city and image quality [ 34 – 37 ]. Three-dimensional sonography allows a more accurate calculation of the uterine volume. It also allows a more precise estimation of endometrial morphology and volume. Endometrial volume and morphology are the most crucial factors for IVF success. Nonoptimal endometrial lining or a small endometrial volume impacts embryo implantation. In these cases, it might be prudent to consider embryo cryopreser­vation and opt for a cryocycle [ 38 ]. In addition, 3D techniques such as 3D Doppler enable the visualization of endometrial blood fl ow and neo­vascularization of cervical carcinomas, which are completely beyond the scope of conventional 2D US.
Imaging modes such as the glass-body mode are the most optimal for the recognition of tumor­feeding vessels. The glass-body mode is a very good method for hysterosalpingo-contrast­sonography (HyCoSy) to detect abnormal vari­cosity in the adnexal region. The use of 3D US dramatically facilitates HyCoSy and provides a better assessment of tubal patency [ 39 ]. Furthermore, 3D US techniques enable an estimation of the ovarian reserve and can be applied during follicle monitoring [ 40 ]. Thus, particular automated systems such as the
2 Principles of 3D Ultrasound
23
Fig. 2.2 3D image of a uterine myoma (Voluson E8)
Fig. 2.3 3D image of uterus arcuatus (Voluson E8)