CS 152 Computer Architecture and Engineering Lecture 9 -- Memory 2014-2-18 John Lazzaro (not a prof - “John” is always OK) TA: Eric Love www-inst.eecs.berkeley.edu/~cs152/ Play: CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM chip capacity: from 1Kb (1971) to 4Gb (2013) CS 152 L14: Cache I UC Regents Spring 2005 © UCB Gordon Moore UCB B.S. Chemistry 1950. CS 152 L9: Memory UC Regents Spring 2014 © UCB CS 152 L9: Memory UC Regents Spring 2014 © UCB Today: State Storage Tools on Silicon ICs Capacitance: Holds state as charge Transistors: How to move charge DRAM: 1 Transistor + 1 Capacitor Architecture: Arrays and interfaces VLSI == “Very Large Scale Integration” The tall thin designer, with feet on the ground and head in the sky. The ground: Physics and IC Fabrication The sky: Architecture and Applications CS 152 L9: Memory Carver Mead UC Regents Spring 2014 © UCB Today’s Lecture: DRAM DRAM: Bottom-up DRAM: Top-down DRAM: Systems CS 152 L9: Memory UC Regents Spring 2014 © UCB Capacitance and memory Intel Micron 8 GB NAND flash device, 2 bit per cell, 25 nm minimum feature, 16.5 mm by 10.1 mm. CS 152 L14: Cache I UC Regents Spring 2005 © UCB Recall: Building a capacitor Top Plate Dielectric Bottom Plate CS 152 L9: Memory Conducts electricity well. (metal, doped polysilicon) An insulator. Does not conducts electricity at all. (air, glass (silicon dioxide)) Conducts electricity well (metal, doped polysilicon) UC Regents Spring 2014 © UCB Recall: Capacitors in action Because the dielectric is an insulator, and does not conduct. ++++++ I=0 --- --- After circuit “settles” ... Q = C V = C * 1.5 Volts (D cell) Q: Charge stored on capacitor C: The capacitance of the device: function of device shape and type of dielectric. 1.5V After battery is removed: ++++++ Still, Q = C * 1.5 Volts --- --Capacitor “remembers” charge CS 152 L9: Memory UC Regents Spring 2014 © UCB Storing computational state as charge State is coded as the amount of energy stored by a device. ++++++ --- --- 1.5V ++++++ --- --- State is read by sensing the amount of energy Problems: noise changes Q (up or down), parasitics leak or source Q. Fortunately, Q cannot change instantaneously, but that only gets us in the ballpark. CS 152 L9: Memory UC Regents Spring 2014 © UCB How do we fight noise and win? Store more energy than we expect from the noise. Q = CV. To store more charge, use a bigger V or make a bigger C. Cost: Power, chip size. Example: 1 bit per capacitor. Represent state Write 1.5 volts on as charge in ways that To C.read C, measure V. are robust to noise. V > 0.75 volts is a “1”. V < 0.75 volts is a “0”. Cost: Could have stored many bits on that capacitor. Correct small state errors thatEx: read C every 1 ms Is V > 0.75 volts? are introduced by noise. Write back 1.5V Cost: Complexity. (yes) or 0V (no). CS 152 L9: Memory UC Regents Spring 2014 © UCB MOS Transistors Two diodes and a capacitor in an interesting arrangement. So, we begin with a diode review ... CS 152 L9: Memory UC Regents Spring 2014 © UCB Diodes in action ... Resistor Light emitting diode (LED) Light on? Yes! Light on? No! CS 152 L9: Memory UC Regents Spring 2014 © UCB Diodes: Current vs Voltage Diode is off I ≈ - Io Anode + I Diode is on I ≈ Io exp(V/Vo) V Cathode I = Io [exp(V/Vo) - 1] Io range: 1fA to 1nA CS 152 L9: Memory Vo range: 25mV to 60 mV UC Regents Spring 2014 © UCB Making a diode on a silicon wafer CS 152 L9: Memory UC Regents Spring 2014 © UCB A pure (”intrinsic”) silicon crystal ... Conducts electricity better than an insulator, worse than a conductor. Why? Most electrons (dots) are in a full “valence” band. Moving in the band is difficult. Especially near 0 degrees Lots of room, K. but few electrons. Forbidden “band gap” CS 152 L9: Memory Conduction band Valence band Many electrons, but packed too tight to e l e c t r o n e n e r g y UC Regents Spring 2014 © UCB Intrinsic silicon crystal as T rises ... Some valence band electrons diffuse into the conduction band. These electrons leave behind “holes” in the valence band, allowing remaining electrons to move easier. More electrons, better conduction CS 152 L9: Memory Conduction band Valence band We think of “holes” as positive carriers ... e l e c t r o n e n e r g y UC Regents Spring 2014 © UCB We “engineer” crystal with impurities ... CS 152 L9: Memory UC Regents Spring 2014 © UCB N-type silicon: add donor atoms Use diffusion or ion implantation to replace some of the Si atoms with As Arsensic has an extra electron that is “donates” to the conduction band. n+ : heavy doping. n- : light doping. Electrons from donor atoms. Improves conductivy. CS 152 L9: Memory Conduction band Donor energy Valence band No change in the number of holes e l e c t r o n e n e r g y UC Regents Spring 2014 © UCB P-type silicon: add acceptor atoms Use diffusion or ion implantation to replace some of the Si atoms with Boron Boron has one fewer electron than Si. It can accept valence band electrons, creating holes. p+ : heavy doping. p- : light doping. No change in conduction band electron count Conduction band Acceptor energy Valence band Number of holes increased, conductivity CS 152 L9: Memory e l e c t r o n e n e r g y UC Regents Spring 2014 © UCB How to make a silicon diode ... Wafer cross-section Cathode: - - n+ V p- Anode: + + pregion Wafer doped p-type depletion At V ≈ 0, “hill” too high for electrons to diffuse region up. n+ region no carriers For holes, going “downhill” is hard. V controls hill. CS 152 L9: Memory depletion region e l e c t r o n e n e r g y UC Regents Spring 2014 © UCB Diodes: Current vs Voltage Diode is off I ≈ - Io Anode + I Diode is on I ≈ Io exp(V/Vo) V Cathode I = Io [exp(V/Vo) - 1] Io range: 1fA to 1nA CS 152 L9: Memory Vo range: 25mV to 60 mV UC Regents Spring 2014 © UCB Note: IC Diodes are biased “off”! V1 V2 V1 V2 n+ n+ p0 V - “ground” V1, V2 > 0V. Diodes “off”, only current is Io “leakage”. I = Io [exp(V/Vo) - 1] Anodes of all diodes on wafer connected to ground. CS 152 L9: Memory UC Regents Spring 2014 © UCB MOS Transistors Two diodes and a capacitor in an interesting arrangement ... CS 152 L9: Memory UC Regents Spring 2014 © UCB What we want: the perfect switch. V1 Switch is off. V1 is not connected to V2. p- We want to turn a p-type region into an n-type region under voltage control. Switch is on. V1 is connected to V2. We need electrons to fill valence holes and add conduction band electrons n+ V1 V2 n+ n+ V2 ++++++ p- --- --CS 152 L9: Memory UC Regents Spring 2014 © UCB An n-channel MOS transistor (nFET) Vg = 0V Vd = 1V I ≈ nA n+ Vs = 0V Polysilicon gate, dielectric n+ dielectric, and substrate form a capacitor. pnFet is off (I is “leakage”) Vg = 1V Vd = 1V +++++++++ I ≈ μA dielectric ------------------n+ pCS 152 L9: Memory Vs = 0V n+ Vg = 1V, small region near the surface turns from p-type to ntype. nFet is on UC Regents Spring 2014 © UCB Mask set for an n-Fet (circa 1986) Vg = 0V Vd = 1V I ≈ nA n+ dielectric n+ p- Top-down view: CS 152 L9: Memory Vs = 0V Masks #1: n+ diffusion #2: poly (gate) #3: diff contact #4: metal Layers to do p-Fet not shown. Modern processes have 6 to 10 metal layers (or more) (in 1986: 2). UC Regents Spring 2014 © UCB “Design rules” for masks, 1986 ... Poly overhang. So that if masks are misaligned , we still get “---” in channel. Minimum gate length. So that the source and drain depletion regions do not meet! length #1: n+ diffusion #2: poly (gate) CS 152 L9: Memory Metal rules: Contact separation from channel, one fixed contact size, overlap rules with metal, etc ... #3: diff contact #4: metal UC Regents Spring 2014 © UCB Fabrication CS 250 L1: Fab/Design Interface UC Regents Fall 2013 © UCB Mask set for an n-Fet ... Vg = 1V Vd = 1V I ≈ μA n+ Vd Vs = 0V dielectric n+ Vg Ids Vs pMasks Top-down view: CS 152 L11: VLSI #1: n+ diffusion #2: poly (gate) #3: diff contact #4: metal How does a fab use a mask set to make an IC? UC Regents Fall 2006 © UCB Start with an un-doped wafer ... UV hardens exposed resist. A wafe wash leaves only hard resist. oxide p- Steps #1: dope wafer p- #2: grow gate oxide #3: grow undoped polysilicon #4: spin on photoresist CS 152 L11: VLSI #5: place positive poly mask and expose with UV. UC Regents Fall 2006 © UCB Wet etch to remove unmasked ... HF acid etches through poly and oxide, but not hardened resist. oxide p- oxide After etch and resist removal pCS 152 L11: VLSI UC Regents Fall 2006 © UCB Use diffusion mask to implant n-type accelerated donor atoms oxide n+ n+ p- CS 152 L11: VLSI Notice how donor atoms are blocked by gate and do not enter channel. Thus, the channel is “selfaligned”, precise mask alignment is not needed! UC Regents Fall 2006 © UCB Metallization completes device oxide n+ n+ p- oxide n+ n+ p- oxide n+ n+ p- CS 152 L11: VLSI Grow a thick oxide on top of the wafer. Mask and etch to make contact holes Put a layer of metal on chip. Be sure to fill in the holes! UC Regents Fall 2006 © UCB Final product ... Vd Vs oxide n+ n+ p- Top-down view: CS 152 L11: VLSI “The planar process” Jean Hoerni, Fairchild Semiconductor 1958 UC Regents Fall 2006 © UCB p-channel Transistors CS 152 L11: VLSI UC Regents Fall 2006 © UCB p-Fet: Change polarity of everything Vwell = Vs = 1V I ≈ μA p+ Vg = 0V Vs Vd = 0V dielectric p+ n-well p- New “n-well” mask Vg Isd Vd “Mobility” of holes is slower than electrons. p-Fets drive less current than nFets, all else being equal CS 152 L11: VLSI UC Regents Fall 2006 © UCB Dynamic Memory Cells CS 152 L9: Memory UC Regents Spring 2014 © UCB Recall: Capacitors in action Because the dielectric is an insulator, and does not conduct. ++++++ I=0 --- --- After circuit “settles” ... Q = C V = C * 1.5 Volts (D cell) Q: Charge stored on capacitor C: The capacitance of the device: function of device shape and type of dielectric. 1.5V After battery is removed: ++++++ Still, Q = C * 1.5 Volts --- --Capacitor “remembers” charge CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM cell: 1 transistor, 1 capacitor “Bit Line” “Word Line” Vdd Word Line Vdd Capacitor “Bit Line” “Bit Line” oxide n+ oxide n+ ------ pWord Line and Vdd run on “z-axis” CS 152 L9: Memory Why Vcap values start out at ground. Vdd Vcap Diode leakage current. UC Regents Spring 2014 © UCB A 4 x 4 DRAM array (16 bits) .... CS 152 L9: Memory UC Regents Spring 2014 © UCB Invented after SRAM, by Robert Dennard CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Circuit Challenge #1: Writing Vdd Vdd Vgs + + + + + + + Vdd Vc Vdd - Vth. Bad, we store less charge. Q. Why do we not get Vdd? Because NFETs ,only pass “0” kA.[Vgs -Vth]^2 well. Ids = but “turns off” when Vgs <= Vgs = Vdd - Vc. When Vdd - Vc == Vth, charging effectively Vth! stops! CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Challenge #2: Destructive Reads +++++++ (stored charge from Bit Line cell) Word Line + (initialized + + to a low + + Vdd voltage) + + 0 -> Vdd Vc -> 0 Raising the word line removes the charge from every cell it connects to! DRAMs write back after each read. CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Circuit Challenge #3a: Sensing Assume Ccell = 1 fF Bit line may have 2000 nFet drains, assume bit line C of 100 fF, or 100*Ccell 100*Ccell. Ccell holds Q = Ccell*(Vdd-Vth) When we dump this charge onto Ccell the bit line, what voltage do we see? dV = [Ccell*(Vdd-Vth)] / [100*Ccell] dV = (Vdd-Vth) / 100 ≈ tens of millivolts! In practice, scale array to get a 60mV signal. CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Circuit Challenge #3b: Sensing ... How do we reliably sense a 60mV signal? Compare the bit line against the voltage on a “dummy” bit line. “sense Bit line to sense + amp” ? “Dummy” bit line. Dummy bit line Cells hold no charge. CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Challenge #4: Leakage ... Bit Line Word Line + + + + + + + Vdd Parasitic currents leak away charge. Solution: “Refresh”, by rewriting cells at regular intervals (tens of milliseconds) oxide n+ ------ n+ pCS 152 L9: Memory oxide Diode leakage ... UC Regents Spring 2014 © UCB DRAM Challenge #5: Cosmic Rays ... Bit Line Word Line + + + + + + + Vdd This cell capacitor holds 25,000 electrons (today, less). Cosmic rays that constantly bombard us can release Solution: Store extra bits to detect and the charge! correct random bit flips (ECC). oxide n+ ------ n+ pCS 152 L9: Memory oxide Cosmic ray hit. UC Regents Spring 2014 © UCB DRAM Challenge 6: Yield If one bit is bad, do we throw chip away? ... Solution: add extra bit lines (i.e. 80 when you only need 64). During testing, find the bad bit lines, and use high current to Extra bit lines. Used for “sparing”. burn away “fuses” put on chip to remove them. CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM Challenge 7: Scaling Recall: Process Scaling (“Moore’s Law”) Due to reducing V and C (length and width of Cs decrease, but plate distance gets smaller). Recent slope more shallow because V is being scaled From: “Facing the Hot Chips Challenge Again”, Bill Holt, Intel, presented at Hot Chips 17, 2005. CS 152 L9: Memory lessUC Regents Spring 2014 © UCB DRAM Challenge 7: Scaling Each generation of IC technology, we shrink width and length of cell. If Ccell and drain capacitances scale together, number of bits per bit line stays constant. dV ≈ 60 mV= [Ccell*(Vdd-Vth)] / [100*Ccell] Problem 1: Number of arrays per chip grows! Problem 2: Vdd may need to scale down too! Solution: Constant Innovation of Cell CS 152 L9: Memory UC Regents Spring 2014 © UCB Poly-diffusion Ccell is ancient history “Bit Line” “Word Line” Vdd Word Line Vdd Capacitor “Bit Line” “Bit Line” oxide oxide n+ ------ n+ p- Word Line and Vdd run on “z-axis” CS 152 L9: Memory UC Regents Spring 2014 © UCB Early replacement: “Trench” capacitors CS 152 L9: Memory UC Regents Spring 2014 © UCB Final generation of trench capacitors The companies that kept scaling trench capacitors for commodity DRAM chips went out of business. CS 152 L14: Cache I UC Regents Spring 2005 © UCB Modern cells: “stacked” capacitors CS 152 L9: Memory UC Regents Spring 2014 © UCB Micron 50nm 1-Gbit DDR2 die photo CS 152 L9: Memory UC Regents Spring 2014 © UCB Samsung 90nm stacked capacitor bitcell. DRAM: the field for material and process innovation ArabindaCSDas 152 L14: Cache I UC Regents Spring 2005 © UCB Cell access transistors for the 4 leading vendors Chipmakers turn to new process for sub-nm DRAM cells Jeongdong CS Choe, 152 L14: TechInsights Cache I UC Regents Spring 2005 © UCB Samsung 30nm From JSSC, and Arabinda Das CS 152 L14: Cache I UC Regents Spring 2005 © UCB In the labs: Vertical cell transistors ... CS 152 L9: Memory UC Regents Spring 2014 © UCB Break Play: CS 152 L9: Memory UC Regents Spring 2014 © UCB Today’s Lecture: DRAM DRAM: Bottom-up DRAM: Top-down DRAM: Systems CS 152 L9: Memory UC Regents Spring 2014 © UCB Memory Arrays CS 152 L9: Memory UC Regents Spring 2014 © UCB Bit Line “Column” “Word Line” “Row” People buy DRAM for the bits. “Edge” circuits are overhead. CS 152 L9: Memory So, we amortize the edge circuits over big arrays. UC Regents Spring 2014 © UCB A “bank” of 128 Mb (512Mb chip -> 4 banks) 1 13-bit row address input of In reality, 16384 columns are divided into 64 smaller arrays. 81 92 de co de r 16384 columns 8192 rows 134 217 728 usable bits (tester found good bits in bigger array) 16384 bits delivered by sense amps Select requested bits, send off the chip CS 152 L9: Memory UC Regents Spring 2014 © UCB Recall DRAM Challenge #3b: Sensing How do we reliably sense a 60mV signal? Compare the bit line against the voltage on a “dummy” bit line. [...] “sense Bit line to sense + amp” ? “Dummy” bit line. Dummy bit line Cells hold no charge. CS 152 L9: Memory UC Regents Spring 2014 © UCB “Sensing” is row read into sense amps Slow! This 2.5ns period DRAM (400 MT/s) can do row reads at only 55 ns ( 18 MHz). 1 13-bit row address input of 81 92 DRAM has high latency to first bit out. A fact of life de co de r 16384 columns 8192 rows 134 217 728 usable bits (tester found good bits in bigger array) 16384 bits delivered by sense amps Select requested bits, send off the chip CS 152 L9: Memory UC Regents Spring 2014 © UCB An ill-timed refresh may add to latency Bit Line Word Line + + + + + + + Vdd Parasitic currents leak away charge. Solution: “Refresh”, by rewriting cells at regular intervals (tens of milliseconds) oxide n+ ------ n+ pCS 152 L9: Memory oxide Diode leakage ... UC Regents Spring 2014 © UCB Latency is not the same as bandwidth! Thus, push to faster DRAM interfaces 1 13-bit row address input of 81 92 de co de r What if we want all of the 16384 bits? In row access time (55 ns) we can do 22 transfers at 400 MT/s. 16-bit chip bus -> 22 x 16 = 352 bits << Now the row access 16384time looks fast! 16384 columns 8192 rows 134 217 728 usable bits (tester found good bits in bigger array) 16384 bits delivered by sense amps Select requested bits, send off the CS 152 L9: Memory UC Regents Spring 2014 © UCB Sadly, it’s rarely this good ... 1 13-bit row address input of 81 92 de co de r What if we want all of the 16384 bits? The “we” for a CPU would be the program running on the CPU. Recall Amdalh’s law: If 20% of the memory accesses need a new row access ... not good. 16384 columns 8192 rows 134 217 728 usable bits (tester found good bits in bigger array) 16384 bits delivered by sense amps Select requested bits, send off the CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM latency/bandwidth chip features Columns: Design the right interface for CPUs to request the subset of a column of data it wishes: 16384 bits delivered by sense amps Select requested bits, send off the chip Interleaving: Design the right interface to the 4 memory banks on the chip, so several row requests run in parallel. Bank 1 CS 152 L9: Memory Bank 2 Bank 3 Bank 4 UC Regents Spring 2014 © UCB Off-chip interface for the Micron part ... A clocked bus: 200 MHz clock, data transfers on both edges (DDR). DRAM is controlled via commands (READ, WRITE, REFRESH, ...) CS 152 L9: Memory Note! This example is best-case! To access a new row, a slow ACTIVE command must run before the READ. Synchronous data output. UC Regents Spring 2014 © UCB Opening a row before reading 15 ns CS 152 L9: Memory Auto-Precharge ... READ 15 ns 55 ns between row opens. UC Regents Spring 2014 © UCB However, we can read columns quickly Note: This is a “normal read” (not Auto-Precharge). Both READs are to the same bank, but different columns. CS 152 L9: Memory UC Regents Spring 2014 © UCB Why can we read columns quickly? 1 13-bit row address input Column reads select from the 16384 bits here of 81 92 de co de r 16384 columns 8192 rows 134 217 728 usable bits (tester found good bits in bigger array) 16384 bits delivered by sense amps Select requested bits, send off the chip CS 152 L9: Memory UC Regents Spring 2014 © UCB Interleave: Access all 4 banks in parallel Interleaving: Design the right interface to the 4 memory banks on the chip, so several row requests run in parallel. Bank a Bank b Bank c Bank d Can also do other commands on banks concurrently. CS 152 L9: Memory UC Regents Spring 2014 © UCB Only part of a bigger story ... CS 152 L9: Memory UC Regents Spring 2014 © UCB Only part of a bigger story ... CS 152 L9: Memory UC Regents Spring 2014 © UCB DRAM controllers: reorder requests From: CS 152 L9: Memory UC Regents Spring 2014 © UCB Today’s Lecture: DRAM DRAM: Bottom-up DRAM: Top-down DRAM: Systems CS 152 L9: Memory UC Regents Spring 2014 © UCB Installing a Dual Inline Memory Module (DIMM) CS 152 L14: Cache I UC Regents Spring 2005 © UCB DDR2 SO-DIMM Module DRAM chips are wired in parallel and run in lockstep. CS 152 L9: Memory UC Regents Spring 2014 © UCB From DRAM chip to DIMM module ... Each RAM chip responsible for 8 lines of the 64 bit data bus (U5 holds the check bits). Commands sent to all 9 chips, qualified by per-chip select lines. CS 152 L9: Memory UC Regents Spring 2014 © UCB How DIMMs talk to CPU Integrated Memory Controller (IMC) On the same die as CPU. SDRAM bus: Parallel bus with a single master. CS 152 L9: Memory UC Regents Spring 2014 © UCB Intel Core i5: Sandy Bridge All on chip: x86 cores GPU North Bridge DRAM controller CS 152 L9: Memory On chip ring network UC Regents Spring 2014 © UCB Lower levels of DRAM bus specification Transaction Protocols Signal Timing on Wires Wires Electrical Properties Mechanical Properties Ideally, DIMMs made by any manufacturer should fit into any compliant socket, and work. CS 152 L9: Memory UC Regents Spring 2014 © UCB Upper levels of DRAM bus specification Collaboration between DRAM manufacturers (Samsung, Micron) and DRAM users (Intel, Cisco, ... ). Transaction Protocols Signal Timing on Wires Wires Electrical Properties Mechanical Properties CS 152 L9: Memory UC Regents Spring 2014 © UCB Bus wires shared between many DIMMS Apple Xserve G5 - has 8 DIMM slots, to support 8GB. DIMMs respond to transaction requests. Since memory controller is the only bus master, and there are a small number of DIMM slots, bus sharing is easy: use DIMMselect signal wires to each slot. Memory controller is the only “bus master” - it can start transactions on the bus, but the DIMMs cannot. CS 152 L9: Memory UC Regents Spring 2014 © UCB Sony PS 4 Uses graphics DRAM for all 8GB of RAM (very high bandwidth). 4 core Jaguar x86 176 GB/s Mem BW 1152 GPU Cores 1.84 TeraFLOP Tradeoff: GDDR5 chips connect to CPU with dedicated wires. Not via a shared bus. More system pins, thus higher cost. 4 core Jaguar x86 Focus is on “serious gamer” not “media center”. 5.5 GHz GDDR5 MacBook Air ... too thin to use DIMMs CS 152 L9: Memory UC Regents Spring 2014 © UCB Mainboard: fills about battery 25% of ... the laptop Non-removable, “form-fit” 35 W-h battery: Fills most of the volume ... CS 152 L9: Memory UC Regents Spring 2014 © UCB Macbook Air Top Core i5: CPU + DRAM controller Bottom 4GB DRAM soldered to the main board CS 152 L9: Memory UC Regents Spring 2014 © UCB CS 152 L14: Cache I UC Regents Spring 2005 © UCB Original iPad (2010) “Package-in-Package” 128MB SDRAM dies (2) Apple A4 SoC Cut-away side view Dies connect using bond wires and solder balls ... CS 152 L14: Cache I UC Regents Spring 2005 © UCB 3-D memory stack Thru-silicon-vias (TSVs) CS 152 L9: Memory UC Regents Spring 2014 © UCB Sony Playstation Vita ... CS 152 L14: Cache I UC Regents Spring 2005 © UCB 1 Gb Samsung Wide I/O DRAM + Toshiba/Sony ARM CPU 1080 pads with 40 µm spacing, face-to-face. “Face-to-face” limits this scheme to two chips, but avoids thru-silicon-vias (TSVs). CS 152 L14: Cache I UC Regents Spring 2005 © UCB On Thursday Caching, part one ... Have fun in section !