- •Preface
- •Contributors
- •Contents
- •Introduction
- •Literature Review
- •Major Issues
- •Major Studies
- •Negative Studies
- •References
- •1.1.1 Introduction
- •1.1.3 Torsional Ultrasound
- •1.1.4 Our Procedure for Emulsifying the Nucleus
- •References
- •1.2 Transitioning to Bimanual MICS
- •1.2.1 Introduction
- •1.2.2 Technique
- •1.2.3 Summary
- •1.3 0.7 mm Microincision Cataract Surgery
- •1.3.1 Sub 1 mm MICS: Why?
- •1.3.3 Instrumentation
- •1.3.3.2 0.7 mm Irrigating Instruments
- •1.3.4 Surgery
- •1.3.4.1 Incision
- •1.3.4.2 Capsulorhexis
- •1.3.4.3 Hydrodissection
- •1.3.4.4 Prechopping
- •1.3.5 0.7 mm MICS Combined Procedures
- •1.3.5.1 0.7 mm MICS and Glaucoma Surgery
- •1.3.6 Summary
- •References
- •2. MICS Instrumentation
- •2.1 MICS Instrument Choice: The First Step in the Transition
- •2.2 MICS Incision
- •2.3 MICS Capsulorhexis
- •2.4 MICS Prechopping
- •2.5 MICS Irrigation/Aspiration Instruments
- •2.5.1 19 G Instruments
- •2.5.2 21 G Instruments
- •2.6 MICS Auxiliary Instrument
- •2.6.1 Scissors
- •2.6.2 Gas Forced Infusion
- •2.6.3 Surge Prevention
- •2.7 New MICS Instruments
- •2.7.1 Flat Instruments
- •References
- •3.1 Introduction
- •3.2 Power Generation
- •3.3.1 Tuning
- •3.2.2 Phaco Energy
- •3.2.2.1 Low Frequency Energy
- •3.2.2.2 High Frequency Energy
- •3.2.3 Transient Cavitation
- •3.2.4 Sustained Cavitation
- •3.3.1 Alteration of Stroke Length
- •3.3.2 Alteration of Duration
- •3.3.2.1 Burst Mode
- •3.3.2.2 Pulse Mode
- •Micro Pulse (Hyper-Pulse)
- •Pulse Shaping
- •3.3.3 Alteration of Emission
- •3.4 Fluidics
- •3.5 Vacuum Sources
- •3.6 Surge
- •3.7.1 Micro-incisional Phaco
- •3.7.2 Bimanual Micro-Incisional Phaco
- •3.7.3 Micro-Incisional Coaxial Phaco
- •3.7.3.1 Irrigation and Aspiration
- •3.8 Conclusion
- •Reference
- •Further Reading
- •4.1 Introduction
- •4.3 Incision Size
- •4.4 Torsional Ultrasound
- •4.5 Conclusion
- •References
- •5. Technology Available
- •5.1 How to Better Use Fluidics with MICS
- •5.1.1 Physical Considerations
- •5.1.1.2 Chamber Stability
- •5.1.1.3 Holdability
- •5.1.2 Surgical Considerations
- •5.1.2.2 Phaco Technique
- •5.1.2.4 The OS3 and CataRhex SwissTech Platforms
- •Equipment
- •Machine Settings
- •5.2 How to Use Power Modulation in MICS
- •5.2.1 Introduction
- •5.2.3 The Concept of Unoccluded Flow Vacuum
- •5.2.4 The Intricacies of Ultrasound Power Modulation
- •5.2.5 The Variable Incidence of Wound Burn Rates
- •References
- •5.3 MICS with Different Platforms
- •5.3.1 MICS with the Accurus Surgical System
- •5.3.1.1 Introduction and Historic Background
- •5.3.1.3 Surgical Parameters for MICS with Accurus
- •5.3.1.4 Final Considerations
- •5.3.2.1 Introduction
- •5.3.2.7 Technology for MICS on the AMO Signature
- •5.3.2.8 Applying Signature Technology to CMICS and BMICS
- •5.3.3 MICS with Different Platforms: Stellaris Vision Enhancement System
- •5.3.3.2 Evaluating the Stellaris Vision Enhancement System
- •5.3.3.3 The Advantages of BMICS
- •References
- •6.1 Pupil Dilation and Preoperative Preparation
- •6.1.1 Managing the Small Pupil
- •6.1.2 Techniques that Depend on the Manipulation of the Pupil
- •6.1.3 Iris Surgery
- •6.1.4 Preoperative Preparation and Infection Prophylaxis
- •6.1.5 Evaluating Risk
- •6.1.6 Assessing Your Approach
- •6.1.7 Preventing Infection, Step by Step
- •6.1.8 Sample Protocol Outline
- •6.1.9 A Careful, Critical Eye
- •References
- •6.2 Incisions
- •References
- •6.3 Thermodynamics
- •6.3.1 Introduction
- •6.3.2 Corneal Thermal Damage
- •6.3.3 Heat Generation
- •6.3.4 Factors that Contribute to Thermal Incision Damage
- •6.3.4.1 Energy Emission: Amount and Pattern of How the Energy Is Delivered
- •6.3.4.3 Viscoelastic Devices and Possible Occlusion of the Aspiration Line
- •6.3.4.4 Irrigation Flow
- •6.3.4.5 Position of the Tip Inside the Incision
- •6.3.4.6 Tip Design
- •6.3.4.7 Surgical Technique
- •6.3.5 Conclusion
- •6.4 Using Ophthalmic Viscosurgical Devices with Smaller Incisions
- •6.4.1 Introduction
- •6.4.1.1 The Nature of OVDs: Rheology
- •6.4.1.3 Soft Shell and Ultimate Soft Shell Technique (SST & USST)
- •6.4.2 Routine, Special and complicated Cases
- •6.4.2.1 Phakic and Anterior Chamber IOLs
- •6.4.2.3 Fuchs’ Endothelial Dystrophy
- •6.4.2.5 Capsular Staining for White & Black Cataracts
- •6.4.2.6 Flomax® Intraoperative Floppy Iris Syndrome USST
- •6.4.3 Discussion
- •References
- •6.5 Capsulorhexis
- •References
- •References
- •6.7 Biaxial Microincision Cataract Surgery: Techniques and Sample Surgical Parameters
- •6.8.1 Surgical Technique
- •6.8.2 Advantages
- •6.8.3 Disadvantages
- •6.8.4 Final Thoughts
- •References
- •6.9 BiMICS vs. CoMICS: Our Actual Technique (Bimanual Micro Cataract Surgery vs. Coaxial Micro Cataract Surgery)
- •6.9.1 Introduction
- •6.9.2 Historical Background
- •6.9.3 BiMICS. BiManual MicroIncision Cataract Surgery
- •6.9.3.1 Introduction
- •6.9.3.2 Instrumentation
- •6.9.3.5 Phacotips
- •6.9.3.6 Capsulorhexis
- •6.9.3.7 Phaco Knives
- •6.9.3.8 The Phaco Machines
- •6.9.3.9 Phaco Pumps
- •6.9.3.10 Ultrasound Power Delivery
- •6.9.3.11 IOL Implantation
- •6.9.3.12 Astigmatism
- •6.9.4.1 Capsulorhexis
- •6.9.4.2 Phacotips
- •6.9.4.3 The Phaco Machines
- •6.9.4.4 Phaco Pumps
- •6.9.4.5 Ultrasound Power Delivery
- •6.9.4.6 Irrigation-Aspiration
- •6.9.4.7 Incision-Assisted IOL Implantation
- •6.9.5 Conclusion
- •References
- •6.10 Endophthalmitis Prevention
- •6.10.1 Antibiotic Prophylaxis
- •6.10.2 Wound Construction
- •6.10.3 Summary
- •References
- •7.1 High Myopia
- •7.2 Posterior Polar Cataract
- •7.3 Posterior Subluxed Cataracts
- •7.4 Mature Cataract with Zonular Dialysis
- •7.5 Punctured Posterior Capsule
- •7.6 Posterior Capsule Rupture
- •7.7 Pseudoexfoliation
- •7.8 Rock-Hard Nuclei
- •7.9 Switching Hands
- •7.10 Microcornea or Microphthalmos
- •7.11 Large Iridodialysis and Zonular Defects
- •7.12 Intraoperative Floppy Iris Syndrome (IFIS)
- •7.14 Iris Bombé
- •7.15 Very Shallow Anterior Chambers
- •7.16 Refractive Lens Exchange
- •7.18 Intraocular Cautery
- •7.19 Biaxial Microincision Instruments
- •References
- •7.1 MICS in Special Cases: Incomplete Capsulorhexis
- •7.1.1 Introduction
- •7.1.2 Avoiding Complications While Constructing Your Microcapsulorhexis
- •7.1.3 Avoiding Complications During Biaxial Phaco with an Incomplete Capsulorhexis
- •7.1.4 Avoiding Complications During IOL Insertion with an Incomplete Capsulorhexis
- •7.1.5 Conclusions
- •References
- •7.2 MICS in Special Cases (on CD): Vitreous Loss
- •7.2.1 Introduction
- •7.2.2 Posterior Capsule Tears and Vitreous Prolapse
- •7.2.3 Vitreous and the Epinucleus or Cortex
- •7.2.4 Different Techniques Other than Pars Plana Vitrectomy for Nuclear Loss in Vitreous
- •7.2.5 Pars Plana Vitrectomy
- •7.2.6 Zonulolysis
- •References
- •7.3 How to Deal with Very Hard and Intumescent Cataracts
- •7.3.1 Introduction
- •7.3.2 Types of Cataracts
- •7.3.3 Management of Hard Cataracts Through Biaxial Technique
- •7.3.4 Incision
- •7.3.5 Capsulorrhexis
- •7.3.6 Hydrodissection
- •7.3.8 Conclusion
- •References
- •8. IOL Types and Implantation Techniques
- •8.1 MICS Intraocular Lenses
- •8.1.1 Introduction
- •8.1.2 Lenses
- •8.1.2.2 ThinOptX MICS IOLs (ThinOptX, Abingdon, VA)
- •8.1.2.3 Akreos MI60 AO Micro Incision IOL (Bausch & Lomb, Rochester, NY)
- •8.1.2.4 IOLtech MICS lens (IOLtech, La Rochelle, France; and Carl Zeiss Meditec, Stuttgard, Germany)
- •8.1.3 Optical Quality of MICS IOLs
- •8.1.4 Conclusion
- •References
- •8.2 Implantation Techniques
- •8.2.2 Prerequisites to a Sub-2 Injection
- •8.2.3 IOLs Used for Injection Through Microincision
- •8.2.3.1 Material
- •8.2.3.2 Design
- •8.2.3.3 Optic Design
- •8.2.3.4 Haptic Design
- •8.2.3.5 Posterior Barrier (360°)
- •8.2.4 Injectors Meant for Microincision
- •8.2.4.1 Objectives of Injectors Meant for Microincision
- •8.2.4.2 Characteristics of Sub-2 Injectors
- •8.2.4.3 The Cartridges
- •Loading Chambers
- •Injection Tunnels and Cartridge Tips
- •8.2.4.4 The Plunger Tips (or plunger)
- •8.2.4.5 Pushing Systems
- •8.2.4.6 Injector Bodies
- •8.2.4.7 Principal Sub-2 Injectors
- •8.2.5 Visco Elastic Substances and Injection Through Microincision
- •8.2.6 Techniques of Sub-2 Injection
- •8.2.6.2 Incision Construction
- •8.2.6.3 Pressurization of the Anterior Chamber
- •8.2.6.4 Loading the Cartridge
- •8.2.6.5 Loading the Injector
- •8.2.6.6 Insertion of the Plunger Tip
- •8.2.6.7 Injection in the Anterior Chamber
- •8.2.6.8 Positioning the IOL in the Capsular Bag
- •8.2.6.9 Removing the VES
- •8.2.6.10 Thin Roller Injector
- •8.2.6.11 Conclusion
- •Reference
- •8.3 Special Lenses
- •8.3.1 Toric Posterior Chamber Intraocular Lenses in Cataract Surgery and Refractive Lens Exchange
- •8.3.1.1 Introduction
- •8.3.1.3 T-IOL Calculation
- •8.3.1.4 Current T-IOL Models
- •8.3.1.5 Preoperative Marking
- •8.3.1.6 Clinical Indications
- •8.3.1.7 Custom-Made Lenses
- •8.3.1.8 Conclusion for Practice
- •References
- •8.3.2 Special Lenses: MF
- •8.3.2.1 Discussion
- •8.3.2.2 Conclusion
- •8.3.2.3 Outlook
- •References
- •8.3.3 Special Lenses: Aspheric
- •References
- •8.3.4 Intraocular Lenses to Restore and Preserve Vision Following Cataract Surgery
- •8.3.4.1 Introduction
- •8.3.4.2 Why Filter Blue Light?
- •Summary
- •8.3.4.3 Importance of Blue Light to Cataract and Refractive Lens Exchange Patients
- •Summary
- •8.3.4.4 Quality of Vision with Blue Light Filtering IOLs
- •Summary
- •8.3.4.5 Clinical Experience
- •Summary
- •8.3.4.6 Unresolved Issues and Future Considerations
- •References
- •8.3.5 Microincision Intraocular Lenses: Others
- •8.3.5.1 ThinOptX®
- •8.3.5.2 Smart IOL
- •8.3.5.4 AcriTec
- •8.3.5.5 Akreos
- •8.3.5.7 Rayner
- •8.3.5.8 Injectable Polymers
- •8.3.5.9 Final Comments
- •References
- •9. Outcomes
- •9.1 Safety: MICS versus Coaxial Phaco
- •9.1.1 Introduction
- •9.1.2 Visual Outcomes
- •9.1.3 Incision Damage
- •9.1.4 Corneal Incision Burn
- •9.1.5 Corneal Changes
- •9.1.6 Infection
- •9.1.7 Summary
- •References
- •9.2 Control of Corneal Astigmatism and Aberrations
- •9.2.1 Introduction: Impacts of MICS Incision on the Outcomes of Cataract Surgery
- •9.2.2 Objective Evaluation of Corneal Incision
- •9.2.3 Control of Corneal Aberration and Astigmatism with MICS
- •9.2.4 Role of Corneal Aberrometry in Evaluating MICS Incision
- •9.2.5 Role of OCT in Evaluating MICS Incision
- •9.2.6 Our Experience in Corneal Aberrations and Astigmatism After MICS
- •9.2.7 Conclusion
- •References
- •9.3 Corneal Endothelium and Other Safety Issues
- •9.4 Incision Quality in MICS
- •9.4.1 Introduction: History of Incision Size Reduction
- •9.4.2 The Trends Towards Microincision Cataract Surgery (BMICS)
- •9.4.3 Advantages of Minimizing the Incision Size
- •9.4.4 Model for the Analysis of Corneal Incision Quality [21]
- •9.4.5 Our Protocol for Evaluation of Incision Quality in BMICS [21]
- •9.4.6 Results
- •9.4.6.1 Visual, Refractive and Biomicroscopic Outcomes
- •9.4.6.2 Incision Imaging (OCT) Outcomes
- •9.4.8 Conclusion
- •References
- •INDEX
38 |
W. J. Fishkind |
at its resonant frequency. For example, the resistance of the aqueous is less than the resistance of the cortex, which in turn, is less than the resistance of the nucleus. As the resistance to the phaco tip varies, to maintain maximum efficiency, depending on the machine, small alterations in frequency or stroke length are created by the tuning circuitry in the CPU. This is important to minimize the excessive generation of ultrasonic energy, which is harmful to the intraocular contents. The surgeon will subjectively determine good tuning circuitry by a sense of smoothness and power.
3.2.2 Phaco Energy
The actual tangible forces that emulsify the nucleus are thought to be a blend of the “Jackhammer” energy and cavitational energy. The “jackhammer” energy is the physical striking of the needle against the nucleus. Cavitational energy generation is more convoluted. Recent studies indicate that there are two kinds of cavitational energy: low frequency energy and high frequency energy.
3.2.2.1 Low Frequency Energy
Low frequency energy is the frequency of energy that is selected by the manufacturer for the individual machine. As noted above, it is generally 27–50 Hz. It is omni directional and will reflect from surfaces such as the cornea or sclera. It travels over great distances and has no cavitational impact. It is, however, the engine that generates cavitational bubbles. These are the fuel for high frequency energy.
3.2.2.2 High Frequency Energy
Low frequency energy is the dynamic force to generate high frequency energy. When the needle, moving at the lower frequency, excites implosion of cavitational bubbles, high frequency energy is created. In its powerful configuration, transient cavitation will generate a 1-mm cone of energy extending up to 10 mm. from the phaco tip. In its inactive form, sustained cavitation does nothing more than vibrating the cavitational bubbles.
3.2.3 Transient Cavitation
The phaco needle, moving through a liquid medium at ultrasonic speeds, gives rise to intense zones of high and low pressure. Low pressure, created with the backward movement of the tip, pulls dissolved gases out of the solution, thus producing micro bubbles. Forward tip movement then creates an equally intense zone of high pressure. This initiates compression of the micro bubbles until they implode. At the moment of implosion, the bubbles create a temperature of 7,204°C and a shock wave of 5,171,100 mbar. Of the micro bubbles created, 75% implode, amassing to create a powerful shock wave, radiating from the phaco tip perpendicular to the bevel of the phaco tip with annular spread.
However, 25% of the bubbles are too large to implode. These micro bubbles are swept up in the shock wave and radiated with it. Transient cavitation is a violent event. The energy created by transient cavitation exists for not more than 4 ms and extends from the phaco tip in a cone shape distribution, in the immediate vicinity of the phaco tip, and within its lumen. It is this form of cavitation that is thought to generate the energy responsible for emulsification of cataractous material (Fig. 3.1). Additionally transient cavitation is instrumental in clearing nuclear fragments within the phaco needle preventing repetitive needle clogging.
The transient cavitational energy can be directed in any desired direction. The angle of the bevel of the
Fig. 3.1 The micro bubbles are visible at the phaco tip. The micro void around the phaco tip is replenished with fresh BSS providing fuel for transient cavitation
3 Evolution of Ultrasound Pumps and Fluidics and Ultrasound Power |
39 |
phaco needle governs the direction of the generation of shock wave and micro bubbles.
3.2.4 Sustained Cavitation
If phaco is energized beyond 4ms, transient cavitation, with generation of micro bubbles and shock waves, ends. The bubbles then begin to vibrate, without implosion.
No shock wave is generated. Therefore, other than mechanical energy, no cavitation energy is produced. Sustained cavitation is ineffective for emulsification (Fig. 3.2a).
a
Fig. 3.2 (a) Transient cavitation energy is shown in
blue, stabilized cavitational b energy shown in red.
Continuous power: Only the initial energy is transient. The remaining is stabilized energy. In a 50-ms pulse, only the initial 4 ms are transient. In micro pulse phaco, the entire pulse is transient energy. (b) The x-axis represents time and the y-axis millivolts. The blue tracing shows the low power (mv) created during continuous phaco. This is stabilized cavitation. The red tracing represents shorts bursts of high power (mv) generated during whitestar phaco. This is transient cavitation
Water bath, hydrophonic studies indicate that transient cavitation is significantly more powerful than sustained cavitation (Fig. 3.2b). With this information in mind, it would appear that continuous phaco is best used to emulsify the intact nucleus, held in place by the capsular bag, during the sculpting phase of divide and conquer or stop and chop. In this setting, jackhammer energy is most important for emulsification.
Transient cavitation is maximized during micro pulse phaco. This is best used during phaco of the nuclear fragments in the later phase of the above two procedures, or during phaco chop procedures [1].
