Federated Learning With Quantized Global Model Updates

Mohammad Mohammadi Amiri, Deniz Gunduz, Sanjeev R. Kulkarni, H. Vincent Poor

Introduction

Federated learning (FL) enables wireless devices to collaboratively train a global model by utilizing locally available data and computational capabilities under the coordination of a parameter server (PS) while the data never leaves the devices .

FL mainly targets mobile applications at the network edge, and the wireless communication links connecting these devices to the network are typically limited in bandwidth and power, and suffer from various channel impairments such as fading, shadowing, or interference; hence the need to develop an FL framework with limited communication requirements becomes more vital. While communication-efficient FL has been widely studied, prior works mainly focused on the devices-to-PS links, assuming perfect broadcasting of the global model to the devices at each iteration. In this paper, we design an FL algorithm aiming to reduce the cost of both PS-to-device and devices-to-PS communications. To address the importance of quantization at the PS-to-device direction, we highlight that some devices simply may not have the sufficient bandwidth to receive the global model update when the model size is relatively large, particularly in the wireless setting, where the devices are away from the base station. This would result in consistent exclusion of these devices, resulting in significant performance loss. Moreover, the impact of quantization in the device-to-PS direction is less severe due to the impact of averaging local updates at the PS.

There is a fast-growing body of literature on the communication efficiency of FL targeting restricted bandwidth devices. Several studies address this issue by considering communications with rate limitations, and propose different compression and quantization techniques , as well as performing local updates to reduce the frequency of communications from the devices to the PS . Statistical challenges arise in FL since the data samples may not be independent and identically distributed (iid) across devices. The common sources of the dependence or bias in data distribution are the participating devices being located in a particular geographic region, and/or at a particular time window . Different approaches have been studied to mitigate the effect of non-iid data in FL . Also, FL suffers from a significant variability in the system, which is mainly due to the hardware, network connectivity, and available power associated with different devices . Active device selection schemes have been introduced to alleviate significant variability in FL systems, where a subset of devices share the resources and participate at each iteration of training . There have also been efforts in developing convergence guarantees for FL under various scenarios, considering iid data across the devices , non-iid data , participation of all the devices , or only a subset of devices at each iteration , and FL under limited communication constraints . Furthermore, FL with compressed global model transmission has been studied recently in aiming to alleviate the communication footprint from the PS to the devices. Since the global model parameters are relatively skewed/diverse, with the scheme in at each iteration the PS employs a linear transform before quantization, and the devices apply the inverse linear transform to estimate the global model. On the other hand, error compensation at the PS is employed in to accumulate the error of quantizing the global model.

Our contributions

With the exception of , the literature on FL considers perfect broadcasting of the global model from the PS to the devices. With this assumption, no matter what type of local update or device-to-PS communication strategy is used, all the devices are synchronized with the same global model at each iteration. In this paper, we instead consider broadcasting a quantized version of the global model update by the PS, which provides the devices with a lossy estimate of the global model (rather than its accurate estimate) with which to perform local training. This further reduces the communication cost of FL, which can be particularly limited for transmission over a wireless medium while serving a massive number of devices. Also, it is interesting to investigate the impact of various hyperparameters on the performance of FL with lossy broadcasting of the global model since FL involves transmission over wireless networks with limited bandwidth. We introduce a lossy FL (LFL) algorithm, where at each iteration the PS broadcasts a compressed version of the global model update to all the devices through quantization. To be precise, the PS exploits the knowledge of the last global model estimate available at the devices as side information to quantize the global model update. The devices recover an estimate of the current global model by combining the received quantized global model update with their previous estimate, and perform local training using their estimate, and return the local model updates, again employing quantization. The PS updates the global model after receiving the quantized local model updates from the devices. We provide convergence analysis of the LFL algorithm investigating the impact of lossy broadcasting on the performance of FL, where for ease of analysis we assume the availability of accurate local model updates from the devices at the PS. Numerical experiments on the MNIST and CIFAR-10 datasets illustrate the efficiency of the proposed LFL algorithm. We observe that the proposed LFL scheme, which leads to a significant communication cost saving, provides a promising performance with no visible gap to the performance of the fully lossless scenario where the communication from both PS-to-device and device-to-PS directions is assumed to be perfect. Also, it is illustrated that the proposed LFL scheme significantly outperforms the schemes introduced in and considering compression from the PS to devices.

We highlight that the proposed LFL algorithm differs from the approaches introduced in , where the PS sends a quantized version of the current global model to a subset of devices that will participate in the learning process at that iteration. The efficiency of quantization diminishes significantly when the peak-to-average ratio of the parameters is large. To overcome this, in the PS first employs a linear transform in order to spread the information of the global model vector more evenly among its dimensions, and broadcasts a quantized version of the resultant vector. Furthermore, in the PS broadcasts quantized global model with error accumulation to compensate the quantization error. Instead, we propose broadcasting the global model update, with respect to the previous estimate at the devices, rather than the global model itself. We remark that the global model update has less variability/variance and peak-to-average ratio than the global model, and hence, for the same communication load, the devices can have a more accurate estimate of the global model. However, this would require all the devices to track the global model at each iteration, even if they do not participate in the learning process by sending their local update. We argue that broadcasting the global model update to the whole set of devices, rather than a randomly chosen subset, would introduce limited additional communication cost as broadcasting is typically more efficient than sending independent information to devices. Moreover, in practice, the subset of participating devices remain the same for a number of iterations, until a device leaves or joins. Our algorithm can easily be adopted to such scenarios by sending the global model, rather than the model update, every time the subset of devices changes. Note also that, compared to the LFL algorithm, the approach introduced in requires a significantly higher computational overhead due to employing the linear transform at the PS and its inverse at the devices, where this overhead grows with the size of the model parameters. Furthermore, the performance evaluation in is limited to the experimental results, while in this paper we provide an in-depth convergence analysis of the proposed LFL algorithm. The advantage of the proposed LFL algorithm over the approaches introduced in is shown numerically, where, despite its significantly smaller communication load, it provides considerably higher accuracy. This illustrates that quantizing the global model update provides a more accurate global model estimate at the devices than quantizing the global model itself.

Notation

Lossy Federated Learning (LFL) Algorithm

We consider a lossy PS-to-device transmission, in which the PS sends a compressed version of the global model to the devices. This reduces the communication cost, and can be particularly beneficial when the PS resources are limited, and/or communication takes place over a constrained bandwidth medium. We denote the estimate of the global model θ(t){\boldsymbol{\theta}}(t) at the devices by \hstretch2\hstretch.5θ^(t)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t), where tt represents the global iteration count. Having recovered \hstretch2\hstretch.5θ^(t)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t), the devices perform a τ\tau-step SGD with respect to their local datasets, and transmit their local model updates to the PS using quantization while accumulating the quantization error.

In the proposed LFL algorithm, the PS performs stochastic quantization similarly to the QSGD algorithm introduced in with a slight modification to broadcast the information about the global model to the devices. In particular, at global iteration tt, the PS aims to broadcast the global model update θ(t)−\hstretch2\hstretch.5θ^(t−1)\boldsymbol{\theta}(t)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t-1) to the devices. We present the stochastic quantization technique we use, denoted by Q(⋅,⋅)Q(\cdot,\cdot), in Appendix A.

For the quantization function φ(x,q)\varphi\left(x,q\right) and vector Q(x,q)\boldsymbol{Q}(\boldsymbol{x},q) given in (18b) and (19), respectively, we have

The proof of Lemma 1 is provided in Appendix B. We highlight that the value of ε\varepsilon depends on the skewness of the magnitudes of the entries of x\boldsymbol{x}, where it increases for a more skewed entries with a higher variance. We have ε=0\varepsilon=0, if and only if all the entries of x\boldsymbol{x} have the same magnitude, and ε=1\varepsilon=1, if and only if x\boldsymbol{x} has only one non-zero entry.

Given a quantization level q1q_{1}, the PS broadcasts \boldsymbol{Q}\big{(}\boldsymbol{\theta}(t)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t-1),q_{1}\big{)} to the devices at global iteration tt. Then the devices obtain the following estimate of θ(t)\boldsymbol{\theta}(t):

which is equivalent to \hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t)={\boldsymbol{\theta}}(0)+\sum\nolimits_{i=1}^{t}\boldsymbol{Q}\big{(}\boldsymbol{\theta}(i)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(i-1),q_{1}\big{)}, where we assumed that \hstretch2\hstretch.5θ^(0)=θ(0)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(0)={\boldsymbol{\theta}}(0). We note that, having the knowledge of the compressed vector \boldsymbol{Q}\big{(}\boldsymbol{\theta}(i)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(i-1),q_{1}\big{)}, ∀i∈[t]\forall i\in[t], the PS can also track \hstretch2\hstretch.5θ^(t)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t) at each iteration.

2 Local Update Aggregation

After recovering \hstretch2\hstretch.5θ^(t)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t), device mm performs a τ\tau-step local SGD, where the ii-th step corresponds to θmi+1(t)=θmi(t)−ηmi(t)∇Fm(θmi(t),ξmi(t))\boldsymbol{\theta}_{m}^{i+1}(t)=\boldsymbol{\theta}_{m}^{i}(t)-\eta^{i}_{m}(t)\nabla F_{m}\left(\boldsymbol{\theta}_{m}^{i}(t),\xi_{m}^{i}(t)\right), i∈[τ]i\in[\tau], where θm1(t)=\hstretch2\hstretch.5θ^(t)\boldsymbol{\theta}_{m}^{1}(t)=\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t), and ξmi(t)\xi_{m}^{i}(t) denotes the local mini-batch chosen uniformly at random from the local dataset Bm\mathcal{B}_{m}. It then aims to transmit local model update Δθm(t)=θmτ+1(t)−\hstretch2\hstretch.5θ^(t)\Delta\boldsymbol{\theta}_{m}(t)=\boldsymbol{\theta}_{m}^{\tau+1}(t)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t) through quantization with error compensation. It performs quantization after error compensation accumulating the quantization error, and transmits \boldsymbol{Q}\big{(}\Delta\boldsymbol{\theta}_{m}(t)+\boldsymbol{\delta}_{m}(t),q_{2}\big{)} using a quantization level q2q_{2}, where δm(t)\boldsymbol{\delta}_{m}(t) retains the quantization error, and is updated as

where we set δm(0)=0\boldsymbol{\delta}_{m}(0)=\boldsymbol{0}. Having received \boldsymbol{Q}\big{(}\Delta\boldsymbol{\theta}_{m}(t)+\boldsymbol{\delta}_{m}(t),q_{2}\big{)} from device mm, ∀m∈[M]\forall m\in[M], the PS updates the global model as

Algorithm 1 summarizes the proposed LFL algorithm.

We do not consider error compensation at the PS with LFL since we have observed performance degradation numerically when compensating the quantization error at the PS. We argue that LFL naturally accumulates the quantization error at the PS since it sends the quatized global model update with respect to the last global model estimate at the devices. We further highlight that the proposed approach is not limited to any specific quantization technique, and any compression technique can be used within the proposed framework.

Convergence Analysis of LFL Algorithm

Here we analyze the convergence behaviour of LFL, where for simplicity of the analysis, we assume that the devices can transmit their local updates, Δθm(t)\Delta\boldsymbol{\theta}_{m}(t), ∀m\forall m, accurately/in a lossless fashion to the PS, and focus on the impact of lossy broadcasting on the convergence.

We denote the optimal solution minimizing loss function F(θ)F(\boldsymbol{\theta}) by θ∗\boldsymbol{\theta}^{*}, and the minimum loss as F∗F^{*}, i.e., θ∗≜arg⁡min⁡θF(θ)\boldsymbol{\theta}^{*}\triangleq\arg\mathop{\min}\nolimits_{\boldsymbol{\theta}}F(\boldsymbol{\theta}), and F∗≜F(θ∗)F^{*}\triangleq F(\boldsymbol{\theta}^{*}). We also denote the minimum value of the local loss function at device mm by Fm∗F_{m}^{*}. We further define Γ≜F∗−∑m=1MBmBFm∗\Gamma\triangleq F^{*}-\sum\nolimits_{m=1}^{M}\frac{B_{m}}{B}F^{*}_{m}, where Γ≥0\Gamma\geq 0, and its magnitude indicates the bias in the data distribution across devices.

For ease of analysis, we set ηmi(t)=η(t)\eta_{m}^{i}(t)=\eta(t). Thus, the ii-th step SGD at device mm is given by

where θm1(t)=\hstretch2\hstretch.5θ^(t)\boldsymbol{\theta}_{m}^{1}(t)=\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t), given in (2). Device mm transmits the local model update

The expected squared l2l_{2}-norm of the stochastic gradients are bounded, i.e.,

2 Convergence Rate

In the following theorem, whose proof is provided in Appendix C, we present the convergence rate of the LFL algorithm assuming that the devices can send their local updates accurately.

Let 0<\eta(t)\leq\min\big{\{}1,\frac{1}{\mu\tau}\big{\}}, ∀t\forall t. We have

for some 0≤ε≤10\leq\varepsilon\leq 1, and the expectation is with respect to the stochastic gradient function and stochastic quantization.

From the LL-smoothness of the loss function, for 0<\eta(t)\leq\min\big{\{}1,\frac{1}{\mu\tau}\big{\}}, ∀t\forall t, and a total of TT global iterations, it follows that

where the last inequality follows from (11a). Considering η(t)=η\eta(t)=\eta and τ=1\tau=1, we have

Choice of ε𝜀\varepsilon

We highlight that ε\varepsilon appears in the convergence analysis of the LFL algorithm in inequality (E), in which we have

which follows from (23b), where we note that

On average the entries of θ(t)−\hstretch2\hstretch.5θ^(t−1)\boldsymbol{\theta}(t)-\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t-1), given in (15), are not expected to have very diverse magnitudes. Thus, the inequality in (3.2) should hold for a relatively small value of ε\varepsilon. We have observed numerically that ε≈10−3\varepsilon\approx 10^{-3} satisfies inequality (3.2) for the LFL algorithm.

Impact of lossy broadcasting

The first term in B(i)B(i) is due to the imperfect broadcasting of the global model update at the PS, which decreases with q1q_{1} and increases linearly with ε\varepsilon. This term is a complicated function of the number of τ\tau depending on other setting variables.

Numerical Experiments

Here we investigate the performance of the proposed LFL algorithm for image classification on both MNIST and CIFAR-10 datasets utilizing ADAM optimizer . We consider M=40M=40 devices, and we measure the performance as the accuracy with respect to the test samples, called test accuracy.

We train different convolutional neural networks (CNNs) with MNIST and CIFAR-10 datasets. The architectures of these CNNs are described in Table 1.

Data distribution

We consider two data distribution scenarios. In the non-iid scenario, we split the training data samples with the same label (from the same class) to M/10M/10 disjoint subsets (assume that MM is divisible by 10). We then assign each subset of data samples, selected at random, to a different device. In the iid scenario, we randomly split the training data samples to MM disjoint subsets, and assign each subset to a distinct device. We consider non-iid and iid data distributions while training using MNIST and CIFAR-10, respectively.

State-of-the-art approaches

We consider two approaches with lossy broadcasting introduced in and as the state-of-the-art approaches. With the scheme in , referred to as lossy transformed global model (LTGM), the PS first employs a linear transform to project the global model. It then quantizes the resultant vector after the linear transform, and sends the quantized vector to the devices. The devices employ the inverse of the linear transform and use the recovered vector for local training. As suggested in , we consider Walsh-Hadamrd transform and employ the stochastic quantization scheme presented in Appendix A at the PS. On the other hand, with the approach studied in , referred to as lossy global model (LGM), the PS directly quantizes the global model plus the quantization error accumulated from the previous iterations and shares the quantized global model with the devices, while updating the qunatization error. For fairness, we consider the quantization scheme presented in Appendix A with the LGM scheme, and assume the same technique for transmission in the device-to-PS direction introduced in Section 2.2.

Benchmark approaches

We consider the performance of the lossless broadcasting (LB) scenario, where the devices receive the current global model accurately, and perform the quantization with error compensation approach as described in Section 2.2. We highlight that this approach requires transmission of RLB=33dR_{\rm{LB}}=33d bits from the PS, where we assume that each entry of the global model is represented by 3333 bits. Thus, the saving ratio in the communication bits of broadcasting from the PS using LFL versus LB is

where (a) follows assuming that d≫1d\gg 1. We further consider the performance of the fully lossless approach, where in addition to having the accurate global model at the devices, we assume that the PS receives the local model updates from the devices accurately.

In Figure 1 we illustrate the performance of different approaches for non-iid and iid scenarios using MNIST and CIFAR-10, respectively, for training with M=40M=40 devices. Figure 1(a) demonstrates test accuracy of different approaches for non-iid data using MNIST with local mini-batch size ∣ξmi(t)∣=500\left|\xi_{m}^{i}(t)\right|=500 and number of local iterations τ=4\tau=4. We set q2=2q_{2}=2 for all the approaches where the devices perform quantization, and q1=2q_{1}=2 for the LFL and LGM schemes. We observe that the proposed LFL algorithm with (q1,q2)=(2,2)(q_{1},q_{2})=(2,2) performs as good as the fully lossless and LB approaches, despite a factor of 12.7712.77 savings in the number of bits that need to be broadcast compared to the LB approach. This illustrates the efficiency of the LFL algorithm for the iid scenario providing significant communication cost savings without any visible performance degradation. On the other hand, the performance of the LGM algorithm drops after an intermediate number of training iterations, which shows that the quantization level q1=2q_{1}=2 does not provide the devices with an accurate estimate of the global model to rely on for local training. This is particularly more harmful in later iterations as the algorithm approaches the optimal point where a finer estimate of the global model is needed for training. We highlight that the proposed LFL algorithm resolves this deficiency with the LGM algorithm through quantizating the global model update rather than the global model providing a more accurate estimate of the global model to the devices even with a relatively small quantization level q1=2q_{1}=2. Throughout our experiments, we found that the random linear transform with the LTGM scheme is not highly efficient in providing a transformed vector with a relatively small peak-to-average ratio, and the quantization level q1q_{1} should be relatively large to guarantee that the algorithm succeeds in learning. Therefore, we set q1=50q_{1}=50 for the LTGM scheme, which is a relatively large quantization value. The advantage of the proposed LFL algorithm over the LTGM and LGM algorithms for the non-iid scenario can be clearly seen in the figure.

A similar observation is made in Figure 1(b) illustrating the perforance of different approaches for iid data using CIFAR-10 with local mini-batch size ∣ξmi(t)∣=250\left|\xi_{m}^{i}(t)\right|=250 and number of local iterations τ=5\tau=5. The the LFL algorithm with (q1,q2)=(5,3)(q_{1},q_{2})=(5,3) provides ×9.2\times 9.2 smaller communication load compared to LB with q2=3q_{2}=3 without any visible performance degradation with respect to the fully lossless and LB approaches. It also significantly outperforms the LGM algorithm with (q1,q2)=(5,3)(q_{1},q_{2})=(5,3), which shows the advantage of quantizing the global model update rather than the global model for iid data. We also observe that the accuracy level of the LTGM algorithm drops significantly after around 200 global iterations even for a large quantization level q1=1000q_{1}=1000, which shows the deficiency of the linear transform to provide a relatively small peak-to-average ratio for the transformed vector.

Conclusion

FL is demanding in terms of bandwidth, particularly when deep networks with huge numbers of parameters are trained across a large number of devices. Communication is typically the major bottleneck, since it involves iterative transmission over a bandwidth-limited wireless medium between the PS and a massive number of devices at the edge. With the goal of reducing the communication cost, we have studied FL with lossy broadcasting, where, in contrast to most of the existing work in the literature, the PS broadcasts a compressed version of the global model to the devices. We have considered broadcasting quantized global model updates from the PS, which can be used to estimate the current global model at the devices for local SGD iterations. The PS aggregates the quantized local model updates from the devices, according to which it updates the global model. We have derived convergence guarantees for the proposed LFL algorithm to analyze the impact of lossy broadcasting on the FL performance assuming accurate local model updates at the PS. Numerical experiments have shown the efficiency of the proposed LFL algorithm in providing an accurate estimate of the global model to the devices, where it performs as good as the fully lossless and LB approaches for both non-iid and iid data despite the significant reduction in the communication load. It also significantly outperforms the LTGM and LGM algorithms studying compression in the PS-to-device direction thanks to quantizing the global model update rather than the global model at the PS.

References

Appendix A Stochastic quantization

Given a quantization level q≥1q\geq 1, we have

and we highlight that it is represented by

where 6464 bits are used to represent xmaxx_{\rm{max}} and xminx_{\rm{min}}, dd bits are used for sign(xi){\rm{sign}}(x_{i}), ∀i∈[d]\forall i\in[d], and dlog⁡2(q+1)d\log_{2}(q+1) bits represent φ((∣xi∣−xmin)/(xmax−xmin),q)\varphi\left((\left|{x}_{i}\right|-x_{\rm{min}})/(x_{\rm{max}}-x_{\rm{min}}),q\right), ∀i∈[d]\forall i\in[d]. We note that we have modified the QSGD scheme proposed in by normalizing the entries of vector x\boldsymbol{x} with xmax−xminx_{\rm{max}}-x_{\rm{min}} rather than ∥x∥2\left\|\boldsymbol{x}\right\|_{2}.

Appendix B Proof of Lemma 1

Given φ(x,q)\varphi\left(x,q\right) in (18b), we have

where (a) follows since (xq−l)(1−xq+l)≤1/4\left(xq-l\right)\left(1-xq+l\right)\leq 1/4. According to (21), (B) and the definition of Q(x,q)\boldsymbol{Q}(\boldsymbol{x},q) given in (19), it follows that

where (b) follows from (21) and (B), and (c) follows since ε=(xmax−xmin)2/∥x∥22\varepsilon=\left(x_{\rm{max}}-x_{\rm{min}}\right)^{2}/\left\|\boldsymbol{x}\right\|_{2}^{2}.

Appendix C Proof of Theorem 1

In the following, we bound the last two terms on the right hand side (RHS) of (C). From the convexity of ∥⋅∥22\left\|\cdot\right\|_{2}^{2}, it follows that

We rewrite the third term on the RHS of (C) as follows:

By substituting (C) and (2) in (C), it follows that

For \hstretch2\hstretch.5θ^(t)\hstretch{2}{\hat{\hstretch{.5}{\boldsymbol{\theta}}}}(t) given in (2), we have

According to Lemma 3, the inequality in (31) can be rewritten as follows:

Theorem 1 follows from the inequality in (C) having 0<η(t)≤min⁡{1,1μτ}0<\eta(t)\leq\min\left\{1,\frac{1}{\mu\tau}\right\}, ∀t\forall t.

Appendix D Proof of Lemma 2

We first bound the first term on the RHS of (D). We have

where (a) follows from Assumption 3. We have

where (b) follows from the convexity of ∥⋅∥22\left\|\cdot\right\|_{2}^{2} and Assumption 3. Plugging (D) into (D) yields

For the second term on the RHS of (D), we have

where (a) follows from Cauchy-Schwarz inequality. Plugging (D) into (D) yields

where we used the inequality in (D) and η(t)≤1\eta(t)\leq 1. Plugging (D) and (D) into (D) completes the proof of Lemma 2.

Appendix E Proof of Lemma 3

where (a) follows from (23) for some 0≤ε(t)≤10\leq\varepsilon(t)\leq 1 defined as

and in (b) we define ε≜max⁡t{ε(t)}\varepsilon\triangleq\max\nolimits_{t}\{\varepsilon(t)\}. According to (44), from the convexity of ∥⋅∥22\left\|\cdot\right\|^{2}_{2}, it follows that

where (a) follows from Assumption 3. Accordingly, (E) reduces to

Substituting the above inequality into (E) yields